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8/10/2019 TMM 21:10:2014 AlessioCaciagli http://slidepdf.com/reader/full/tmm-21102014-alessiocaciagli 1/27  Alessio Cacia li Laser Particle Acceleration www.hzdr.de HZDR SUMMER STUDENT PROGRAM 2014 A summer well spent playing with big lasers Utrecht, 21.10.2014

TMM 21:10:2014 AlessioCaciagli

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Page 1: TMM 21:10:2014 AlessioCaciagli

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 Alessio Cacia li Laser Particle Acceleration www.hzdr.de 

HZDR SUMMER STUDENT PROGRAM 2014

A summer well spent playing with big lasers

Utrecht, 21.10.2014

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Member of the Helmholtz AssociationPage 2

 Alessio Cacia li Laser Particle Acceleration www.hzdr.de 

Introduction

• Question: where has Alessiobeen during August and

September?

•  Answer: in Germany!

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Introduction

• More precisely… In Dresden! 

• Among other things… Famous forDresden (Messen) porcelain

•  Artistic opinion of a local:

 – Very expensive and… 

 – …Kitch… 

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Introduction

• Question: why was Alessio there?

•  Answer: for a Summer School! – HZDR Summer Student Program

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Introduction

• HZDR is not just a

single building… • Several facilities,

several research fields

 – Energy (materials

efficiency, nuclear

reactors…)  – Health (cancer

research, brain

diseases…) 

 – Matter  (material

science with ion

beams, accelerator

research…) 

My topic:

Laser-Particle Acceleration forCancer therapy application

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Particle Acceleration

How to accelerate particles?

...With big rings and long

corridords (and a lot of

money)

GSI Darmstadt

DESY Hamburg

10 MV/m

Particle are subjected to an

electromagnetic field

They acquire kinetic energy

Higher electric

field (lighter

particles)

Higher kinetic

energies

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Particle Acceleration

How to reach higher kinetic energies?

...With even bigger rings and (an insanely awful lot of) more money

LHC at Geneva

(Switzerland).

Radius: 27 km

(Image: CERN)

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Particle Acceleration

... Maybe there is another (less bloody expensive) way

10.000.000 MV/m

~ mm

High-power laser hitting an aluminum foil target

(DRACO Laser at HZDR, Dresden)

• 106 times bigger electric

field than in a Linear

 Accelerator (LINAC)!

•  Acceleration length: ~mm

against ~km

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Particle Acceleration

100 TW Laser I = 1020 W/cm2  E0 = 1012 V/m

3 J in 30 fs

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Laser Acceleration: Medical application

Why Laser Particle Acceleration?

Laser Driven Proton

Therapy

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Why Laser Particle Acceleration?

 Advantages overconventional

accelerators:

short acceleration length

Laser Acceleration: Medical application

10.000.000 MV/m

~ mm

 Advantages over

conventional cancer

therapy (photontherapy):

Better dose delivery

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

0 10 20 300

1

(175-190 MeV)Protonen

Protonen   N  o  r  m   i  e  r   t  e   D  o  s   i  s

Eindringtiefe in Wasser / cm

Photonen

Normal tissue tumor

   N   o   r   m   a    l   i   z   e    d    d   o   s   e

Depth in water [cm]

Photons

Protons

Protons(175-190 MeV)

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Experimental setup at HZDR: DRACO

 All this stuff is also done in Dresden…

With DRACO

DResden l Aser aCceleration sOurce

In short words…

 A high-power ultra-short-pulses laser

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Experimental setup at HZDR: DRACO

• Power: 150 TW (1012 W)

• Peak Intensity: ~1021

 W/cm2

• Ultra-short pulses: 4J in ~30 fs

• Pulse train: 10 Hz

Initial short pulse

StretcherOscillator (Ti:Sa)

Compressor Target

Area

Power Amplifiers

High-energy

Ultra-short

pulse

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Experimental setup at HZDR:

DRACO

Laser beam

Target

Proton beam

Target alignment!

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My contribution: right in the focus of the

Big Laser

• How to know if you are inthe focus?

 – Use a camera!

In focus Out of focus

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My contribution: right in the focus of the Big Laser

Yes, sometimes

experiment &

computer

models can live

together… 

(even though it’s

a forced

convivence)

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My contribution: right in the focus of the Big Laser

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My contribution: right in the focus of the Big Laser

25 points per minute (was 6…) 

Precision requirement: ± 10 μm 

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Translational Research – Laser Driven Dose Delivery System

Basic research

Clinical practiceLaser driven dose delivery system

Stable & reliable laser protonaccelerator

Precise beam delivery

Real-time dosimetry

Laser / plasmadevelopment

100 

depth in water [cm]

• Proton energy

increase

• Sufficiently

monoenergetic

beam    r   e    l   a   t   i   v   e   e    f    f   e   c   t   i   v   e    d

   o   s   e    [   %    ]

Clinical trials

In vitro- cells

In vivo - animals

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Translational Research – Laser Driven Dose Delivery

System

• Direct comparison of laser driven and conventionally accelerated

protons: no difference between both radiation types

• Dose controlled irradiation (over 4000 shots)

• Relative error of less 10%  clinical precision standard (3-5%)

within reach

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Translational Research – Laser Driven Dose Delivery

System

• Next phase: in vivo irradiations

Main challenge: increase of proton energies to at least 200 MeV

(current is 70 MeV)

Upgrade the laser system

Enhance the effectiveness of acceleration mechanism

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Multiple filamentation of freely

propagating 100 TW beam in air

Thank you for your

attention!

Example of freely

propagating Alessio in the lab

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Laser Acceleration: TNSA

 Acceleration responsible mechanism:

Target-normal sheath acceleration(TNSA)

2. Electron Transport1. Electron Acceleration 3. Electron-proton plasma

expansion

Ion energies: up to 70 MeV

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Laser acceleration: Medical application

I = 1020 W/cm2 

100 TW Laser I = 1020 W/cm2  E0 = 1012 V/m

 Advantage over conventional photon therapy: better dose delivery

0 20 40 60 80 100 

Photon irradiation, 9 fields 

% Dmax

 

12C-ion irradiation, 2 portals 

0 20 40 60 80 100  % Dmax

 

Courtesy: O. Jäkel, DKFZ Heidelberg