Transcript
Page 1: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

1

Master Thesis

The clinical performance of the DAVID-system for the

in vivo verification of VMAT irradiation

Presented by Mustafa Saibu Danpullo

1st supervisor

Prof DrBPoppe

2nd supervisor

Dr HK Looe

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg2

Layout

I Introduction

II Theory

VMAT and IMRT

MLC Design and Agility

MWPC and DAVID system

III Materials amp Methods

Equipment alignment patient data stability of DAVID chamber

Beam property Error detection

Deconvolution

DAVID QA software

IV Results Discussion

V Conclusion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg3

I Introduction

IMRT (Intensity-modulated radiation therapy)

VMAT (Volumetric Modulated Arc Therapy)

Why In vivo verification

ICRU report 24 (1976) recommended that certain types of tumors

requires improve accuracy from 5 to 35

To detect Equipment-related errors and deviations from the initial plan

Complexity of planning and delivery techniques increases risk for

treatment-related error incidents

In 1992 to 2007 more than 4000 near misses without adverse

outcome to patientrsquos case were reported more than 50 were related

to the planning or treatment delivery stage

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg4

In vivo dosimetry methods

in vivo intracavitary dosimetry with TLD

Diodes

DAVID (Device for Advanced Verification of IMRT deliveries

In-vivo verification during treatment

Online measurement of differences in dose to reference

Error detection of the Multi Leaf Collimator (MLC)

I Introduction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

5

II Theory

Mostly Siemens Elekta and Varian have introduced new LINAC

control systems that will be able to change the MLC leaf positions

IMRT uses many small fields to generated by beam-shaping

devices (MLC) to deliver a single dose of radiation

IMRT Intensity-modulated Radiation Therapie

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg6

II TheoryVMAT Volumetric Modulated Arc Therapy

VMAT is a rotational IMRT that can be delivered using

conventional LINAC with MLC

Elekta and Varian have introduced new LINAC control systems

that will be able to change the MLC leaf positions and dose rate

while the gantry is rotating

Precise Beam infinity and Rapid Arc

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg7

A schematic drawing of the Siemens type A Elekta type B and Varian type C MLC [18]

Stepped leafs for different manufacturers [34]

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg8

II Theory Agility MLC design

bull 160 tungsten leafs

bull rounded arc edge

bull 5 mm width

bull High speed(2x normal MLC) of up to

3cmsec

bull large field MLC enable clinicians to

shape radiation

bull extremely low transmission of about

lt05

bull 45 cm isocenter clearance from

accessory holder

MLC Motor

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg9

Inventor

Prof Georges Charpak

France1968

Nobel Prize in Physics (1992)

II Theory Multi wire proportional chamber (MWPC)

The DAVID chamber is a multi-wire

ionization chamber designed by PTW

Freiburg based on Charparks multi wire

proportional chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg10

Compton scattering Electric field causes electrons move to the

anode(wire) and ionizied atomsmolecules to the

cathode(plate)

Each detection wire accumulates charge which

loads a C

After the voltage at the capacitor is read out it is set

to zero and charged again

The voltage achieved is read out by the associated

amplifier at a rate of 1 Hz

Performed by multi-channel electrometer

(MULTIDOS) + additional Software

II Theory DAVID system functioning principle

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 2: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg2

Layout

I Introduction

II Theory

VMAT and IMRT

MLC Design and Agility

MWPC and DAVID system

III Materials amp Methods

Equipment alignment patient data stability of DAVID chamber

Beam property Error detection

Deconvolution

DAVID QA software

IV Results Discussion

V Conclusion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg3

I Introduction

IMRT (Intensity-modulated radiation therapy)

VMAT (Volumetric Modulated Arc Therapy)

Why In vivo verification

ICRU report 24 (1976) recommended that certain types of tumors

requires improve accuracy from 5 to 35

To detect Equipment-related errors and deviations from the initial plan

Complexity of planning and delivery techniques increases risk for

treatment-related error incidents

In 1992 to 2007 more than 4000 near misses without adverse

outcome to patientrsquos case were reported more than 50 were related

to the planning or treatment delivery stage

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg4

In vivo dosimetry methods

in vivo intracavitary dosimetry with TLD

Diodes

DAVID (Device for Advanced Verification of IMRT deliveries

In-vivo verification during treatment

Online measurement of differences in dose to reference

Error detection of the Multi Leaf Collimator (MLC)

I Introduction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

5

II Theory

Mostly Siemens Elekta and Varian have introduced new LINAC

control systems that will be able to change the MLC leaf positions

IMRT uses many small fields to generated by beam-shaping

devices (MLC) to deliver a single dose of radiation

IMRT Intensity-modulated Radiation Therapie

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg6

II TheoryVMAT Volumetric Modulated Arc Therapy

VMAT is a rotational IMRT that can be delivered using

conventional LINAC with MLC

Elekta and Varian have introduced new LINAC control systems

that will be able to change the MLC leaf positions and dose rate

while the gantry is rotating

Precise Beam infinity and Rapid Arc

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg7

A schematic drawing of the Siemens type A Elekta type B and Varian type C MLC [18]

Stepped leafs for different manufacturers [34]

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg8

II Theory Agility MLC design

bull 160 tungsten leafs

bull rounded arc edge

bull 5 mm width

bull High speed(2x normal MLC) of up to

3cmsec

bull large field MLC enable clinicians to

shape radiation

bull extremely low transmission of about

lt05

bull 45 cm isocenter clearance from

accessory holder

MLC Motor

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg9

Inventor

Prof Georges Charpak

France1968

Nobel Prize in Physics (1992)

II Theory Multi wire proportional chamber (MWPC)

The DAVID chamber is a multi-wire

ionization chamber designed by PTW

Freiburg based on Charparks multi wire

proportional chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg10

Compton scattering Electric field causes electrons move to the

anode(wire) and ionizied atomsmolecules to the

cathode(plate)

Each detection wire accumulates charge which

loads a C

After the voltage at the capacitor is read out it is set

to zero and charged again

The voltage achieved is read out by the associated

amplifier at a rate of 1 Hz

Performed by multi-channel electrometer

(MULTIDOS) + additional Software

II Theory DAVID system functioning principle

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 3: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg3

I Introduction

IMRT (Intensity-modulated radiation therapy)

VMAT (Volumetric Modulated Arc Therapy)

Why In vivo verification

ICRU report 24 (1976) recommended that certain types of tumors

requires improve accuracy from 5 to 35

To detect Equipment-related errors and deviations from the initial plan

Complexity of planning and delivery techniques increases risk for

treatment-related error incidents

In 1992 to 2007 more than 4000 near misses without adverse

outcome to patientrsquos case were reported more than 50 were related

to the planning or treatment delivery stage

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg4

In vivo dosimetry methods

in vivo intracavitary dosimetry with TLD

Diodes

DAVID (Device for Advanced Verification of IMRT deliveries

In-vivo verification during treatment

Online measurement of differences in dose to reference

Error detection of the Multi Leaf Collimator (MLC)

I Introduction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

5

II Theory

Mostly Siemens Elekta and Varian have introduced new LINAC

control systems that will be able to change the MLC leaf positions

IMRT uses many small fields to generated by beam-shaping

devices (MLC) to deliver a single dose of radiation

IMRT Intensity-modulated Radiation Therapie

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg6

II TheoryVMAT Volumetric Modulated Arc Therapy

VMAT is a rotational IMRT that can be delivered using

conventional LINAC with MLC

Elekta and Varian have introduced new LINAC control systems

that will be able to change the MLC leaf positions and dose rate

while the gantry is rotating

Precise Beam infinity and Rapid Arc

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg7

A schematic drawing of the Siemens type A Elekta type B and Varian type C MLC [18]

Stepped leafs for different manufacturers [34]

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg8

II Theory Agility MLC design

bull 160 tungsten leafs

bull rounded arc edge

bull 5 mm width

bull High speed(2x normal MLC) of up to

3cmsec

bull large field MLC enable clinicians to

shape radiation

bull extremely low transmission of about

lt05

bull 45 cm isocenter clearance from

accessory holder

MLC Motor

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg9

Inventor

Prof Georges Charpak

France1968

Nobel Prize in Physics (1992)

II Theory Multi wire proportional chamber (MWPC)

The DAVID chamber is a multi-wire

ionization chamber designed by PTW

Freiburg based on Charparks multi wire

proportional chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg10

Compton scattering Electric field causes electrons move to the

anode(wire) and ionizied atomsmolecules to the

cathode(plate)

Each detection wire accumulates charge which

loads a C

After the voltage at the capacitor is read out it is set

to zero and charged again

The voltage achieved is read out by the associated

amplifier at a rate of 1 Hz

Performed by multi-channel electrometer

(MULTIDOS) + additional Software

II Theory DAVID system functioning principle

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 4: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg4

In vivo dosimetry methods

in vivo intracavitary dosimetry with TLD

Diodes

DAVID (Device for Advanced Verification of IMRT deliveries

In-vivo verification during treatment

Online measurement of differences in dose to reference

Error detection of the Multi Leaf Collimator (MLC)

I Introduction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

5

II Theory

Mostly Siemens Elekta and Varian have introduced new LINAC

control systems that will be able to change the MLC leaf positions

IMRT uses many small fields to generated by beam-shaping

devices (MLC) to deliver a single dose of radiation

IMRT Intensity-modulated Radiation Therapie

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg6

II TheoryVMAT Volumetric Modulated Arc Therapy

VMAT is a rotational IMRT that can be delivered using

conventional LINAC with MLC

Elekta and Varian have introduced new LINAC control systems

that will be able to change the MLC leaf positions and dose rate

while the gantry is rotating

Precise Beam infinity and Rapid Arc

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg7

A schematic drawing of the Siemens type A Elekta type B and Varian type C MLC [18]

Stepped leafs for different manufacturers [34]

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg8

II Theory Agility MLC design

bull 160 tungsten leafs

bull rounded arc edge

bull 5 mm width

bull High speed(2x normal MLC) of up to

3cmsec

bull large field MLC enable clinicians to

shape radiation

bull extremely low transmission of about

lt05

bull 45 cm isocenter clearance from

accessory holder

MLC Motor

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg9

Inventor

Prof Georges Charpak

France1968

Nobel Prize in Physics (1992)

II Theory Multi wire proportional chamber (MWPC)

The DAVID chamber is a multi-wire

ionization chamber designed by PTW

Freiburg based on Charparks multi wire

proportional chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg10

Compton scattering Electric field causes electrons move to the

anode(wire) and ionizied atomsmolecules to the

cathode(plate)

Each detection wire accumulates charge which

loads a C

After the voltage at the capacitor is read out it is set

to zero and charged again

The voltage achieved is read out by the associated

amplifier at a rate of 1 Hz

Performed by multi-channel electrometer

(MULTIDOS) + additional Software

II Theory DAVID system functioning principle

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 5: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

5

II Theory

Mostly Siemens Elekta and Varian have introduced new LINAC

control systems that will be able to change the MLC leaf positions

IMRT uses many small fields to generated by beam-shaping

devices (MLC) to deliver a single dose of radiation

IMRT Intensity-modulated Radiation Therapie

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg6

II TheoryVMAT Volumetric Modulated Arc Therapy

VMAT is a rotational IMRT that can be delivered using

conventional LINAC with MLC

Elekta and Varian have introduced new LINAC control systems

that will be able to change the MLC leaf positions and dose rate

while the gantry is rotating

Precise Beam infinity and Rapid Arc

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg7

A schematic drawing of the Siemens type A Elekta type B and Varian type C MLC [18]

Stepped leafs for different manufacturers [34]

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg8

II Theory Agility MLC design

bull 160 tungsten leafs

bull rounded arc edge

bull 5 mm width

bull High speed(2x normal MLC) of up to

3cmsec

bull large field MLC enable clinicians to

shape radiation

bull extremely low transmission of about

lt05

bull 45 cm isocenter clearance from

accessory holder

MLC Motor

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg9

Inventor

Prof Georges Charpak

France1968

Nobel Prize in Physics (1992)

II Theory Multi wire proportional chamber (MWPC)

The DAVID chamber is a multi-wire

ionization chamber designed by PTW

Freiburg based on Charparks multi wire

proportional chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg10

Compton scattering Electric field causes electrons move to the

anode(wire) and ionizied atomsmolecules to the

cathode(plate)

Each detection wire accumulates charge which

loads a C

After the voltage at the capacitor is read out it is set

to zero and charged again

The voltage achieved is read out by the associated

amplifier at a rate of 1 Hz

Performed by multi-channel electrometer

(MULTIDOS) + additional Software

II Theory DAVID system functioning principle

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 6: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg6

II TheoryVMAT Volumetric Modulated Arc Therapy

VMAT is a rotational IMRT that can be delivered using

conventional LINAC with MLC

Elekta and Varian have introduced new LINAC control systems

that will be able to change the MLC leaf positions and dose rate

while the gantry is rotating

Precise Beam infinity and Rapid Arc

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg7

A schematic drawing of the Siemens type A Elekta type B and Varian type C MLC [18]

Stepped leafs for different manufacturers [34]

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg8

II Theory Agility MLC design

bull 160 tungsten leafs

bull rounded arc edge

bull 5 mm width

bull High speed(2x normal MLC) of up to

3cmsec

bull large field MLC enable clinicians to

shape radiation

bull extremely low transmission of about

lt05

bull 45 cm isocenter clearance from

accessory holder

MLC Motor

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg9

Inventor

Prof Georges Charpak

France1968

Nobel Prize in Physics (1992)

II Theory Multi wire proportional chamber (MWPC)

The DAVID chamber is a multi-wire

ionization chamber designed by PTW

Freiburg based on Charparks multi wire

proportional chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg10

Compton scattering Electric field causes electrons move to the

anode(wire) and ionizied atomsmolecules to the

cathode(plate)

Each detection wire accumulates charge which

loads a C

After the voltage at the capacitor is read out it is set

to zero and charged again

The voltage achieved is read out by the associated

amplifier at a rate of 1 Hz

Performed by multi-channel electrometer

(MULTIDOS) + additional Software

II Theory DAVID system functioning principle

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 7: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg7

A schematic drawing of the Siemens type A Elekta type B and Varian type C MLC [18]

Stepped leafs for different manufacturers [34]

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg8

II Theory Agility MLC design

bull 160 tungsten leafs

bull rounded arc edge

bull 5 mm width

bull High speed(2x normal MLC) of up to

3cmsec

bull large field MLC enable clinicians to

shape radiation

bull extremely low transmission of about

lt05

bull 45 cm isocenter clearance from

accessory holder

MLC Motor

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg9

Inventor

Prof Georges Charpak

France1968

Nobel Prize in Physics (1992)

II Theory Multi wire proportional chamber (MWPC)

The DAVID chamber is a multi-wire

ionization chamber designed by PTW

Freiburg based on Charparks multi wire

proportional chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg10

Compton scattering Electric field causes electrons move to the

anode(wire) and ionizied atomsmolecules to the

cathode(plate)

Each detection wire accumulates charge which

loads a C

After the voltage at the capacitor is read out it is set

to zero and charged again

The voltage achieved is read out by the associated

amplifier at a rate of 1 Hz

Performed by multi-channel electrometer

(MULTIDOS) + additional Software

II Theory DAVID system functioning principle

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 8: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg8

II Theory Agility MLC design

bull 160 tungsten leafs

bull rounded arc edge

bull 5 mm width

bull High speed(2x normal MLC) of up to

3cmsec

bull large field MLC enable clinicians to

shape radiation

bull extremely low transmission of about

lt05

bull 45 cm isocenter clearance from

accessory holder

MLC Motor

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg9

Inventor

Prof Georges Charpak

France1968

Nobel Prize in Physics (1992)

II Theory Multi wire proportional chamber (MWPC)

The DAVID chamber is a multi-wire

ionization chamber designed by PTW

Freiburg based on Charparks multi wire

proportional chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg10

Compton scattering Electric field causes electrons move to the

anode(wire) and ionizied atomsmolecules to the

cathode(plate)

Each detection wire accumulates charge which

loads a C

After the voltage at the capacitor is read out it is set

to zero and charged again

The voltage achieved is read out by the associated

amplifier at a rate of 1 Hz

Performed by multi-channel electrometer

(MULTIDOS) + additional Software

II Theory DAVID system functioning principle

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 9: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg9

Inventor

Prof Georges Charpak

France1968

Nobel Prize in Physics (1992)

II Theory Multi wire proportional chamber (MWPC)

The DAVID chamber is a multi-wire

ionization chamber designed by PTW

Freiburg based on Charparks multi wire

proportional chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg10

Compton scattering Electric field causes electrons move to the

anode(wire) and ionizied atomsmolecules to the

cathode(plate)

Each detection wire accumulates charge which

loads a C

After the voltage at the capacitor is read out it is set

to zero and charged again

The voltage achieved is read out by the associated

amplifier at a rate of 1 Hz

Performed by multi-channel electrometer

(MULTIDOS) + additional Software

II Theory DAVID system functioning principle

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 10: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg10

Compton scattering Electric field causes electrons move to the

anode(wire) and ionizied atomsmolecules to the

cathode(plate)

Each detection wire accumulates charge which

loads a C

After the voltage at the capacitor is read out it is set

to zero and charged again

The voltage achieved is read out by the associated

amplifier at a rate of 1 Hz

Performed by multi-channel electrometer

(MULTIDOS) + additional Software

II Theory DAVID system functioning principle

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 11: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

11

Signal interpretation

Ri reading of a single channel (ion charge collected)

C cross section of the lengthy collection volume along the wire

Ii ionization density (x1 start of wire x2 end of wire)

li1-li2 aperture of the associated leave pair

II Theory

II Theory

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 12: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

12

Front Plate

Back Plate

Air Volume

II Theory DAVID system signal recording

3 groups of secondary electrons contributing to the signala)ldquoprimary signalrdquo

b)scattered signal

c)leakage radiation

(background signal)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 13: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg13

VMAT Planning

Treatment Planning System ONCENTRA Masterplan Version 43

ELEKTA Synergy accelerator with an Agility 80 leaf-pair MLC

bull Desktop Pro TM 7011 is Elektas third generation fully integrated

digital control system MOSAIQ DAVID software version 20

DAVID T34065

III Materials and Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 14: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg14

Patient data configuration chart

III Materials amp Methods

Reference

1st session

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 15: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg15

DAVID Analysis

bull PTW DAVID 20 software

III Materials amp Methods

Warning level 3

Alarm level 5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 16: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg16

III Materials amp Methods

bullVMAT 4 (1 HampN 3 Prostates)

bull180deg to -180deg Clockwise and anti clockwise

Stability of the DAVID system

bullIMRT 1 (Prostate)

bull0deg

bull90deg

bull270deg

(Prostate and Head and Neck) 14 days

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 17: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg17

III Materials amp MethodsThe beam property of the DAVID chamber

bullPercentage depth dose (PDD)

bullRoos chamber 34001

bullMP3 water phantom

bullTransmission factor for 6 and 15 MV

bullSemifex T31010 (Diff Field sizes)

Setup conditions

bull With and without DAVID

bull SSD 100 and 80 cm

bull Photon energy 6 and 15

MV

bull Different field sizes

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 18: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg18

1 Successive opening of 1 leaf on 1

side

III Materials amp MethodsVMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 19: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg19

1 Successive opening of 1 leaf on 1

side

VMAT Plan Editing for error detection

bull MATLAB script to change the MLC-positions

3 Field shift of a leaf gap (size of leave

gap remains)

2 Successive shift of a leaf gap (size of

leave gap remains)

III Materials amp Methods

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 20: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg20

DeconvolutionIII Materials amp Methods

S(x) measured signal as convolution of

P(x) True bdquodoseldquo profile with

LRF fɛ(x)

S(x) = P(x) f(x)

bdquovan Cittertldquo iterative deconvolution

algorithm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 21: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg21

opened MLC at every 10th interval from 1st to 80th

pairs

Nine MLC slit through the entire DAVID chamber

IV Results and Discussion Alignment

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 22: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg22

IV Results and Discussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT prostate

bull Deviation of plusmn1 (-1)

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 23: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg23

IV ResultsDiscussion Stability of DAVID System

bull IMRT prostate

bull Deviation of plusmn2 (+2)

bull VMAT HampN

bull Deviation of lt05

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 24: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg24

IV ResultsDiscussion Transmission factor

The average KDAVID

bull 0939 plusmn0003 for 6 MV

and

bull 0953 plusmn 0004 for 15 MV

Reduction of dose at isocenter

due to 8mm of PMMA

By measuring the attenuation

factor the output value can be

corrected

Attenuation of the beam by the DAVID chamber

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 25: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg25

100 cm SSDIncreased about

032 with DAVID

No change of

Dmax

14 cm with

and without DAVID

80 cm SSD

An increased about

426 with DAVID

slight change of

Dmax

13 cm with DAVID

14 cm without DAVID

IV ResultsDiscussion Changes in PDD

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 26: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg26

100 cm SSD

An increased about

067 with DAVID

Dmax

26 cm No change

80 cm SSD

An increased about

18 with DAVID

slight change of

Dmax

18 cm with DAVID

24 cm without DAVID

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 27: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg27

Surface dose

Increase with increase in field size

Increase with increase in energy

Increase with decrease in SSD

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 28: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg28

Pronounce with

decrease in SSD and

increase in photon energy and

increase in field size

Increase in surface dose is

due to scattered secondary

electrons from the DAVID

chamber reaching the

water phantom surface

(electron contamination)

6 cm

45 cm

100 cm

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 29: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg29

Deconvolution test

by iteration method

IV ResultsDiscussion Deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 30: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg30

Deconvolution

bulldoes not depend on the length of the slit

bull40 cm slit results showed a small decrease in the tail signals

10 x 10 cm

10 cm slit

40 cm slit

20 cm slit

30 cm slit

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 31: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

31

IV ResultsDiscussion

Deconvoluted slit signal at 40th and 65th wire

Deconvolution test

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 32: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

32

10x10cm fields before and after deconvolution

Single arc prostate plan before and after deconvolution (3 mm )

IV ResultsDiscussion Deconvolution with DAVID software

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 33: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

33

before deconvolution 61 mm

Gradients of the linear fit

before deconvolution 047 and

after deconvolution 29 mm

Gradients of the linear fit

after deconvolution 094

IV ResultsDiscussion Enhance sensitivity after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 34: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

34

before deconvolution after deconvolution

HampN 6mm error

IV ResultsDiscussion

False alarmwarning effect before deconvolution

The effect is eliminated after deconvolution

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 35: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

35

Undeconvoluted

deconvoluted

Measuring the deconvolution matrix with

the DAVID software as manual LSF of single middle slit is measured and

used to generate the 80x80 LRF matrix with

MAT LAB and installed in the DAVID software

for deconvolution

IV ResultsDiscussion Limitations of DAVID-160 system

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 36: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

36

2mm MLC error single bank shift2mm MLC error single leaf

Analyzing both the maximum deviation

and total deviation in two different plots

at the same time

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 37: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

37

Max Dose 7599GyMax Dose 5727Gc

IV ResultsDiscussion Artificial MLC bang shift Error 2

cm

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 38: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg38

0

1

2

3

4

5

6

7

8

0 8 10 12 14 16 18 20

shift mm

dose

in

cre

ase

G

y

ma

xim

al d

evia

tio

n

Undetectable error Design of the chamber

DAVID Gap-Shift (prostate with OAR rectum back wall)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 39: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

39

DAVID Quality Assurance software (DQA)

MAT LAB 2011b and 2012b

analyzes the daily session for all patients data with 2 clicks online

bull NDD- Non deconvoluted data

bull DD-Deconvoluted data

bull ED- Electrical data

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 40: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

40

Analysis only specific data on

specific date session and only print

out the deconvoluted data (DD)

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 41: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

41

Patient text file from DQA software

Sample patient 2014-01-12

Display only datas with MLC error

indicating the data type (DD)Beam

number Session segment and

particular MLC with error

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 42: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

42

The DQA software displays the warning and alarm errors

Warning and error dialogs at future date entry and invalid date entry respectively

year-month-day `yyyy-mm-dd

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 43: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

43

VMAT and IMRT plans sessions

IV ResultsDiscussion

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 44: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg44

DAVID chamber

bull Linear dependency on leaf opening

bull Sensitivity dependent on leaf gap opening

bull How much radiation pass through the opening

bull Deconvolution double the sensitivity

DAVID is design for specifics LINACS

Independent from the LINAC

In-vivo verification of MLC malfunction during VMAT

bull Undetectability field shifts due to chamber design

(Suggestion perpendicular wires or gradient)

V Conclusions

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 45: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg45

V Conclusion

Single MLC bank shift error

Maximum and total deviation to be analysed

Deconvolution matrix

To be generated for each linac

To be generated by single single slit

bull In comparison to other techniques measurement of undisturbed

signals

-gt no dependence on patient position(EPID)

-gt measurement of the complete delivered dose(TLD diode or MOSFET

detectors)

bull Suggestions for future development Standard design for software

bull Deconvolution program to be integrated

bull DQA to be integrated

bull Design two chambers perpendicular to each other

Co-operate directly with LINAC vendors for specifics designs

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 46: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg46

Sources

1 [1] Ezzel GA Galvin JM Low D Palta JR Rosen I Sharpe MB Xia P Xiao Y Xing L and Yu CX Guidance on delivery

treatment planning and clinical implementation of IMRT report of the IMRT subcommittee of the AAPM radiation

therapy committee Med Phys 2003 302089-115

2 [2] ESTRO Booklet No 9 2008 Guidelines for the verification of IMRT edited by Ben Mijnheer and Dietmar Georg

ISBN 90-804532-9

3 [3] Schneider F Polednik M Wol D Steil V Delana A Wenz F Menegotti L Optimization of the gafchromic EBT

protocol for IMRT QA Z Med Phys 2009 19(1)29-37

4 [4] Poppe B Blechschmidt A Djouguela A Kollho R Rubach A and Harder D Two-dimensional ionisation-chamber

arrays for IMRT plan verication Med Phys 2006 331005-15

5 [5] Poppe B Thieke C Beyer D Kollho R Djouguela A Ruumlhmann A Willborn KC and Harder D DAVID-a translucent

multi-wire transmission ionization chamber for in vivo verication of IMRT and conformal irradiation techniques Phys

Med Biol 2006 511237-48

6 [9] Poppe B Looe H K Chofor N Ruumlhmann A Harder D and Willborn K Clinical Performance of a Transmission

Detector Array for the Permanent Supervision of IMRT Deliveries Radiother Oncol 2010 95158-65

7 [10] Looe H K Harder D Ruumlhmann A Willborn K and Poppe B Enhanced accuracy of the permanent surveillance of

IMRT deliveries by iterative deconvolution of DAVID chamber signal proles Phys Med Biol 2010 553981-92

8 [11] Heukelom S el alWedge factor constituents of high-energy photon beams Head and phantom scatter dose

components Radiother Oncol 32 (1994) 66-3

9 12] Jursinic P A Changes in incident photon uence of 6 and 18 MV x rays caused by blocks and block trays Med

Phys 26 (1999) 2092-8

10 [13] v Klevens H Dependence of the tray transmission factor on collimator setting and sourcesurface distance Med

Phys 27 (2000) 2117-3

11 [14] Sharma SC el al Recommendations for measurement of tray and wedge factors for high energy photons Med

Phys 21 (1994) 573-5

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 47: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg47

Thank you for your

attention

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 48: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg48

Additional Slides

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 49: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

49

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 50: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

Description of the Elekta synergy DAVID160 system

50

David58

David160

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 51: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

51

bullΦ constant with depth

(small interactions)

bullSame electrons set in

motion in each square

bullie interactions per

volume constant through

target

bulldose reaches a

maximum at R (kerma

constant with depth

equals absorbed dose

beyond )

Number of electron tracks set in motion by

photon interaction

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 52: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

52

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 53: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

53

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 54: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

54

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 55: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

55

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56

Page 56: PDF Mustafa_Thesis presentation

WG Medical Radiation Physics Pius-Hospital and Carl von Ossietzky University Oldenburg

56