1
B Grants-in-aid KIBAN-B (FY2014~) https://kaken.nii.ac.jp/d/p/26287055.en.html Magnetic Dipole Moment g-2 Electric Dipole Moment EDM NEW PHYSICS SEARCH Utilize high intensity muon beam of J-PARC Material and Life Science Facility (MLF + How to find T-violation in spin recession signal? • Orbit radius=33.3cm • Cyclotron period=7.4nec Requires 60mrad horizontal kick within 1 cycle Uncertainty for each point is from reading fluctuation of oscilloscope mV 1 Gauss 2 Gauss Grants-in-aid WAKATE-B (FY2011~2013) https://kaken.nii.ac.jp/d/p/ 23740216.en.html R=33.3cm axisymmetrically- excited field E-Gun 110ke V Expected shot in Argon gas. parameters J-PARC original Test exp. Storage field 3 [T] 100 Gauss Beam particle + e - Momentum [MeV/c] 300 0.112 Beam size [rad-m] 1.5×10 -6 3×10 -7 Kick duration[nse c] 300~500 100~300 Cycle period [nsec] 7.4 2.4 Orbit radius 0.33 0.115 Bean line 2m in total This test experiment has been started from 2014. In stead of muon beam, we utilize electron beam from electron gun, Inject electron beam into “Mini-solenoid magnet” and visualize 3- D trajectory, “Mini-solenoid” is 1/3 scale compared to the original storage magnet, but it can apply weak focusing field, We are now beam commissioning, Vertical kicker system will be installed in FY2016. 8 0 c m 60cm [email protected] http://research.kek.jp/people/hiromi/MyHomePage/MiniSolExp.html Amplitude of up-down asymmetry directly indicates non-zero EDM existence!! Noether's (first) theorem Every differentiable symmetry of the action of a physical system has a corresponding conservation law. 3.Charge conjugation parity (CP) violation 2.Charge conjugation is not conserved C C P P No left handed anti- neutrino, nor right handed neutrino Left-handed or right- handed relates to spin C= 1 P= - 1 CP= -1 C=1 P=1 CP=1 The discovery of CP violation in 1964 in the decays of neutral kaons ( weak decay, right picture) ~0.2%! (1964) At least three generations of quarks are required (Cabibbo- Kobayashi-Masukawa Matrix) CP violation Time reversal invariance Anti matte r Weak decay Electric Dipole Moment: EDM Tilt angle=1mrad (0.006degree ) Beam storage plane 3-D Spiral injection does work! “Almost” 2-D orbit (a)Very precise storage magnetic field (1ppm locally) (b)Smooth injection without error field in the storage volume (b)Storage orbit’s plane should be stable <0.01mrad Three keys to detect EDM signal Kicked beam motion in the weak focusing field 3mra d 80mm Kick !! Zoom up Vertical phase space 0.3mr ad 10mm 1.Parity conjugation is not conserved Proton beam (3 GeV, 1MW, 25 Hz) Muon Linac (300 MeV/c) Ultra-Cold + Source and LINAC Laser (2.3 keV/c) (28 MeV/c) Spin dependent decay emits e + in “ + spin direction” Spin=1/2 EDM term can be detected by up-down asymmetry earch for time reversal invariance in muon spi precession Apply MRI technology 3-D spiral injection Kicker and Weak focusing field How to inject muon beam in “MRI” magnet? Usual method (2-D injection) is not applicable, because: Verti cal Kick Storage orbit’s plane 0.66m + Test experiment to demonstrate 3-D spiral injection + beam Iron yoke Engineering design of Super conductive storage magnet is ongoing yoke radius= 2m OPERA 1/8 model H a l f h e i g h t = 1 . 5 m Super conducti ve coils + Apply proper radial fringe field to deflect vertical motion to the horizontal ~ 500nse c ~ 2Gauss Weak focus field at storage volume Weak focus field Development of a pulsed kicker system Mini- solenoid magnet fabricated in 2014 Field measurement is done by hole probe (FY2014) Signal from pickup coil (differential amplifier+ integrator) Current transfer Inner and outer coils 300nsec 80A I(t)=I peak sin(t) Solenoid and radial axes Target region R=33+/- 0.5cm Z=+/-10cm 3H 10W +20k V DC 1M +20kV , 1nF Thyratron switch + G Kicker coil (original size) Signal of CT Picku p coil Signal of Pickup coil Test bench setup High current supply Prof. Nakayam a H. Iinuma My son Aug. 2012 Spatial field is in good agreement between measurement and OPERA simulation! simulati on Momentum and energy conservation Lagrangian is symmetric under continuous translations in space and time But, it is not applicable to quantum field theory Homogeneit y of space-time Angular momentum conservation rotationall y symmetric Spin=1/ 2 Spin dependent angular distribution of Weak decay Weak decay BEYOND STANDARD MODEL & h ttp://g-2.kek. jp S s t cos L R L R 0 L K 0 0 0 L K s c m e d EDM B c B g m e EDM SPIN 2 2 2 B R B F R B v F y B y R B n B y R 0 m E n cm n V H H 27 10 82 . 0 , 2 2 . 1 ~ 3 . 33 , 1 1 2 R r n B B r B B R y y y y 1 n 0 0 v R B F peak kick kick peak B T T B t sin B kick

B Grants-in-aid KIBAN-B (FY2014~) Magnetic Dipole Moment g-2 Electric Dipole Moment EDM Utilize high intensity

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Page 1: B Grants-in-aid KIBAN-B (FY2014~)  Magnetic Dipole Moment g-2 Electric Dipole Moment EDM Utilize high intensity

B

S

stcos

Grants-in-aid KIBAN-B (FY2014~) https://kaken.nii.ac.jp/d/p/26287055.en.html

Magnetic Dipole Moment g-2

Electric Dipole Moment EDM

NEW PHYSICS SEARCH

Utilize high intensity muon beam of J-PARC Material and Life Science Facility (MLF)

+

How to find T-violation in spin recession signal?

• Orbit radius=33.3cm• Cyclotron period=7.4nec• Requires 60mrad

horizontal kick within 1 cycle

Uncertainty for each point is from reading fluctuation of oscilloscope

mV

1 Gauss

2 Gauss

Grants-in-aid WAKATE-B (FY2011~2013)https://kaken.nii.ac.jp/d/p/23740216.en.html

R=33.3cm

axisymmetrically-excited field

E-Gun110keV

Expected shot in Argon gas.

parameters J-PARC original Test exp.

Storage field 3 [T] 100 Gauss Beam particle + e-

Momentum [MeV/c] 300 0.112

Beam size [rad-m]

1.5×10-6 3×10-7

Kick duration[nsec] 300~500 100~300

Cycle period [nsec] 7.4 2.4

Orbit radius [m] 0.33 0.115

Bean line 2m in total

• This test experiment has been started from 2014.

• In stead of muon beam, we utilize electron beam from electron gun,

• Inject electron beam into “Mini-solenoid magnet” and visualize 3-D trajectory,

• “Mini-solenoid” is 1/3 scale compared to the original storage magnet, but it can apply weak focusing field,

• We are now beam commissioning,• Vertical kicker system will be

installed in FY2016.

80cm

60cm

[email protected] http://research.kek.jp/people/hiromi/MyHomePage/MiniSolExp.html

Amplitude of up-down asymmetry directly indicates non-zero EDM existence!!

Noether's (first) theorem Every differentiable symmetry of the action of a physical system has a corresponding conservation law.

3.Charge conjugation parity (CP) violation

2. Charge conjugation is not conserved

L

R

L

R

C

C

PP

• No left handed anti-neutrino, nor right handed neutrino

• Left-handed or right-handed relates to spin

0LK

0

0

0LK

C= 1P= -1CP= -1

C=1P=1CP=1

• The discovery of CP violation in 1964 in the decays of neutral kaons ( weak decay, right picture) ~0.2%! (1964)

• At least three generations of quarks are required (Cabibbo-Kobayashi-Masukawa Matrix)

CP violation Time reversal invariance

Anti matter

Weak decay

Electric Dipole Moment: EDM

scm

ed EDM

BcB

g

m

eEDMSPIN

2

2

2

BTilt angle=1mrad

(0.006degree)

Beam storage plane

3-D Spiral injection does work!

RB F

RB

v

F

yB

“Almost” 2-D orbit

(a)Very precise storage magnetic field (1ppm locally)(b)Smooth injection without error field in the storage volume(b)Storage orbit’s plane should be stable <0.01mrad

Three keys to detect EDM signal

Kicked beam motion in the weak focusing field

3mrad80mm

Kick!!

Zoom up

Vertical phase space

0.3mrad

10mm

1.Parity conjugation is not conserved

Proton beam(3 GeV, 1MW, 25 Hz)

Muon Linac (300 MeV/c)

Ultra-Cold + Source and LINACLaser

(2.3 keV/c) (28 MeV/c)

Spin dependent decay emits e+ in “+ spin direction”

Spin=1/2

EDM term can be detected by up-down asymmetry

Search for time reversal invariance in muon spin precession

Apply MRI technology 3-D spiral injection Kicker and Weak focusing field

How to inject muon beam in “MRI” magnet?

Usual method (2-D injection) is not applicable, because:

yR

BnB y

R0

m

En

cm

n

V

H

H

271082.0

,22.1~

3.33

,11

2

Vertical Kick

R

rnBB

r

B

B

R

yy

y

y

1

n

0

0v

Storage orbit’s plane

0.66m

+

Test experiment to demonstrate 3-D spiral injection

+ beam

Iron yoke

Engineering design of Super conductive storage magnet is ongoing

yoke radius= 2m

OPERA 1/8 model

Half height= 1.5m

Super conductive

coils

RB

+

F

Apply proper radial fringe field to deflect vertical motion to the horizontal

peak

kick

kickpeak

B

T

TBt

sinBkick

~ 500nsec~ 2Gauss

Weak focus field at storage volume

Weak focus field

Development of a pulsed kicker system

Mini-solenoid magnet fabricated in 2014

Field measurement is done by hole probe (FY2014)

Signal from pickup coil (differential amplifier+ integrator)

Current transferInner and outer coils

300nsec

80A

I(t)=Ipeak sin(t)

Solenoid and radial axes

Target region R=33+/-0.5cm

Z=+/-10cm

3H

10W+20kV DC

1M

+20kV , 1nFThyratron switch

+

G

Kicker coil (original size)

Signal of CT

Pickup coil

Signal of Pickup

coil

Test bench setup

High current supply

Prof. Nakayama

H. Iinuma

My son Aug. 2012

Spatial field is in good agreement between measurement and OPERA simulation!

simulation

Momentum and energy conservation

• Lagrangian is symmetric under continuous translations in space and time

• But, it is not applicable to quantum field theory

Homogeneity of space-time

Angular momentum conservation

rotationally symmetric

Spin=1/2

Spin dependent angular distribution of Weak decay

Weak decay

BEYOND STANDARD MODEL &http://g-2.kek.jp