T Violation in n-A Reactions Neutron Optical Parity and - - PowerPoint PPT Presentation

t violation in n a reactions
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T Violation in n-A Reactions Neutron Optical Parity and - - PowerPoint PPT Presentation

page 1 T Violation in n-A Reactions Neutron Optical Parity and Time-Reversal EXperiment Hirohiko M. SHIMIZU Department of Physics, Nagoya University shimizu@phi.phys.nagoya-u.jp on behalf of the NOPTREX collaboration Title(T Violation in n-A


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Title(T Violation in n-A Reactions) Conf(Theoretical Issues and Experimental Opportunities in Searches for Time Reversal Invariance Violation) Date(2018/12/07) At(Amherst)

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Department of Physics, Nagoya University

Hirohiko M. SHIMIZU

shimizu@phi.phys.nagoya-u.jp

T Violation in n-A Reactions

Neutron Optical Parity and Time-Reversal EXperiment

  • n behalf of the NOPTREX collaboration
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Neutron EDM ( )

atomic QCD

Fundamental CP phases

TeV

Energy

nuclear

EDMs of paramagnetic molecules (YbF, PbO, HfF+) Atoms in traps (Tl,Rb,Cs) EDMs of diamagnetic atoms (Hg,Xe,Ra,Rn) EDMs of nuclei and ions (deuteron, etc) Muon EDM

Pospelov Ritz, Ann Phys 318 (05) 119 gluon self-couplings eN couplings

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45h or 2h to reach nEDM “upper limit” (30d or 1d with existing technologies)

nucleon

Neutron EDM ( )

atomic QCD

Fundamental CP phases

TeV

Energy

nuclear

EDMs of paramagnetic molecules (YbF, PbO, HfF+) Atoms in traps (Tl,Rb,Cs) EDMs of diamagnetic atoms (Hg,Xe,Ra,Rn) EDMs of nuclei and ions (deuteron, etc) Muon EDM

Pospelov Ritz, Ann Phys 318 (05) 119 gluon self-couplings eN couplings

compound state experiment

enhanced sensitivity in compound nuclei

NOPTREX Collaboration KEK 2018S12 Neutron Optical Parity and Time Reversal EXperiment

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NOPTREX Collaboration

W.M.Snow, J.Curole, J.Carini

Indiana University

V.Gudkov

  • Univ. South Carolina

B.Plaster, D.Schaper, C.Crawford

Kentucky Univ.

J.D.Bowman, S.Penttila, X.Tong, P.Jiang

Oak Ridge National Lab.

P.Hautle

Paul Scherrer Institut

A.S.Tremsin

  • Univ. California Berkeley

Southern Illinois University

B.M.Goodson M.Veillette

Berea College

KEK 2018S12 Neutron Optical Parity and Time Reversal EXperiment

H.M.Shimizu, M.Kitaguchi, K.Hirota, T.Yamamoto, K.Ishizaki, S.Endoh, T.Sato, Y.Niinomi, T.Morishima, G.Ichikawa, Y.Kiyanagi, J.Hisano, N,Wada, T.Matsushita T.Yoshioka, S.Takada, J.Koga, S.Makise T.Okudaira, K.Sakai, A.Kimura, H.Harada

Nagoya University Kyushu University JAEA

Y.Yamagata, T.Uesaka, K.Tateishi, H.Ikegami

RIKEN

T.Ino, S.Ishimoto, K.Taketani, K.Mishima, C.C.Haddock

KEK

Y.I.Takahashi, M.Hino

Kyoto Univ.

T.Iwata, Y.Miyachi

Yamagata Univ.

T.Momose

  • Univ. British Columbia

Hiroshima Univ.

M.Iinuma

Osaka Univ.

K.Ogata, H.Kohri, M.Yosoi, T.Shima, H.Yoshikawa

Tohoku Univ.

M.Fujita H.Fujioka

Tokyo Inst. Tech.

D.Takahashi

Ashikaga Univ.

R.Ishiguro

Japan Women’s Univ.

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n+139La

140La

(En=0) (En=0.75eV) (En=-48.6eV) 5160.902 keV

absorption cross section total cross section s-wave (l=0) p-wave (l=1)

1eV 1MeV 1keV neutron energy [eV] cross section [b]

(compound nuclei) thermal epithermal fast

Compound States

P-violation

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compound state entrance channel exit channel p-wave s-wave p j=3/2 p j=1/2

P

Universality Check

s j=1/2 mostly unknown

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s-p interference ⇔ channel-spin interference P-odd T-odd

  • rbital

n spin nuclear spin compound nuclear spin n entrance spin channel spin

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compound state exit channel entrance channel p-wave s-wave p 3/2 p 1/2

T

T-odd ➡ Channel-spin Interference

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f = A0 + B0σ · ˆ I + C0σ · ˆ k + D0σ · (ˆ I × ˆ k)

Spin Independent P-even T-even Spin Dependent P-even T-even P-violation P-odd T-even T-violation P-odd T-odd

T-violation in Neutron Optics

fake T-odd negligible

Gudkov, Phys. Rep. 212 (1992) 77

T-violation P-violation

P-violating matrix element

angular momentum factor

T-violating matrix element

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f = A0 + B0σ · ˆ I + C0σ · ˆ k + D0σ · (ˆ I × ˆ k)

Spin Independent P-even T-even Spin Dependent P-even T-even P-violation P-odd T-even Spin Independent P-even T-even T-violation P-odd T-odd Spin Dependent P-even T-even P-violation P-odd T-even T-violation P-odd T-odd

validity of this description can be checked via the consistency among A, B, C

T-violation in Neutron Optics

D≠0 ➡ D’≠0 fake T-odd negligible

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Analyzing Power and Polarization Polarization Transfer Coefficient

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nucleon

12

Neutron EDM ( )

atomic QCD

Fundamental CP phases

TeV

Energy

nuclear

EDMs of paramagnetic molecules (YbF, PbO, HfF+) Atoms in traps (Tl,Rb,Cs) EDMs of diamagnetic atoms (Hg,Xe,Ra,Rn) EDMs of nuclei and ions (deuteron, etc) Muon EDM

Pospelov Ritz, Ann Phys 318 (05) 119 gluon self-couplings eN couplings

compound state experiment

(1) (2) (3) (4)

(n,γ) measurement nuclear theory resonance parameters theory theory

done for 139La done via likelihood analysis V.P.Gudkov

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Y.-H.Song et al., Phys. Rev. C83 (2011) 065503

T-odd P-odd meson couplings

(1), (2) Estimation in Effective Field Theory

~

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Y.H.Song et al., Phys. Rev. C83(2011) 065503 Gudkov, Phys. Rep. 212 (1992) 77 Flambaum, Phys. Rev. C51 (1995) 2914

(1), (2) Estimation in Effective Field Theory

←discovery potential corresponding to the present nEDM upper limit

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[deg] φ

50 100 150 200 250 300 350

)| J ( κ |

3 −

10

2 −

10

1 −

10 1 10

2

10

3

10

kappa_final(x*3.141592653589/180.,[0], [1])

zzzz

139La I=7/2 J=4 131Xe I=3/2 J=1 117Sn I=1/2 J=1 81Br I=3/2 J=2

x2 = Γn

p,j= 1

2

Γn

p

, y2 = Γn

p,j= 3

2

Γn

p

.

κ(J) = ⎧ ⎪ ⎨ ⎪ ⎩ (−1)2I 1 + 1

2

  • 2I−1

I+1 y x

  • (J = I − 1

2)

(−1)2I+1

I I+1

  • 1 − 1

2

  • 2I+3

I y x

  • (J = I + 1

2)

zzzz

x = cos φ, y = sin φ.

zzzz

x2 + y2 = 1

φ : necessary to estimate κ(J)

(3,4) Details of Entrance Channel

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kγ kn σn

(3,4) Details of Entrance Channel

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a0 =

  • Js |V1(Js)|2 +

Js,j |V2(Jpj)|2

a1 = 2Re

Js,Jp,j V1(Js)V 2 (Jpj)P(JsJp 1 2j1IF)

a2 = −2Im

Js,Jp,j V1(Js)V 2 (Jpj)βjP(JsJp 1 2j1IF)

a3 = Re

Js,j,J

p,j V2(Jpj)V

2 (J pj)P(JpJ pjj2IF)3

√ 10

  • 2

1 1

1 2 1 2

2 j j

  • a4

= −Im

Js,j,J

p,j V2(Jpj)V

2 (J pj)P(JpJ pjj2IF)6

√ 5

  • 2

1 1 1

1 2 1 2

2 j j

  • a5

= −Re

  • Js,J

s V1(Jsj)V

1 (J sj)P(JsJ s 1 2 1 21IF) + Jp,j,J

p,j V2(Jpj)V

2 (J pj)P(JpJ pjj1IF)6

  • 1

1 1

1 2 1 2

1 j j

  • a6

= −2Re

Js V1(Jsj)V 2 (Jp = Js, 1 2)

a7 = Re

Js,Jp V1(Js)V 2 (Jp 3 2)P(JsJp 1 2 3 22IF)

a8 = −Re

Jp,j,J

p,j V2(Jpj)V

2 (J pj)P(JpJ pjj1IF)18

  • 2

1 1 1

1 2 1 2

1 j j

  • a9

= −2Re

  • Js,J

s V1(Jsj)V

3 (J sj)P(JsJ s 1 2 1 21IF) + Jp,j,J

p,j V2(Jpj)V

4 (J pj)P(JpJ pjj1IF)6

  • 1

1 1

1 2 1 2

1 j j

  • a10

= −2Re

Js

  • V2(Jp = Js, 1

2)V 3 (Js) + V1(Js)V 4 (Jp = Js, 1 2)

  • a11

= 2Re

Js,Jp

  • V2(Jp 3

2)V 3 (Js) + V1(Js)V 4 (Jp 3 2)

√ 3P(JsJp 1

2 1 32IF)

a12 = −Re

Js,j,J

p,j V2(Jpj)V

4 (J pj)P(JpJ pjj1IF)18

  • 2

1 1 1

1 2 1 2

1 j j

  • a13

= 2Re

  • Js V1(Js)V

3 (Js) + Jpj V2(Jpj)V 4 (Jpj)

  • a14

= 2Re

JsJpj [V2(Jpj)V 3 (Js) + V1(Js)V 4 (Jpj)] P(JsJp 1 2j1IF)

a15 = 2Im

JsJpj [V2(Jpj)V 3 (Js) − V1(Js)V 4 (Jpj)] βjP(JsJp 1 2j1IF)

a16 = 2Re

Jp,j,J

p,j V2(Jpj)V

4 (J pj)P(JpJ pjj2IF)3

√ 10

  • 2

1 1

1 2 1 2

2 j j

  • a17

= −2Im

Jp,j,J

p,j V2(Jpj)V

4 (J pj)P(JpJ pjj2IF)6

√ 5

  • 2

1 1 1

1 2 1 2

2 j j

  • 17

Flambaum, Nucl. Phys. A435 (1985) 352

(3,4) Details of Entrance Channel

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(n,γ)反応を測

A C G

BL04 ANNRI

Ge detector

disk chopper T0 chopper filter collimator

beam stopper

21.5m Ge detector

clustered set

2 clustered sets 7ch ×2 : 14ch 8 coaxial units 8ch Total 22ch

co-axial units

(3,4) Details of Entrance Channel

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19 [us] TOF

1200 1400 1600 1800 2000 2200

[ k e V ]

γ

E

5000 5050 5100 5150 5200 5250

[arbitrary unit]

  • ray yeild

γ

1 2 3 4 5

[eV]

n

E

0.6 0.8 1.2 1.41.6

γ

  • r

a y e n e r g y ( k e V )

N e u t r

  • n

e n e r g y ( e V )

Ground state First, Second excited state Third excited state p-wave resonance

γ-ray yield (arbitrary unit)

139La+n

ground 3- 30 keV 2- 35 keV 5-

140La

63 keV 4- Neutron Energy γ-ray Energy

0.758 eV p-wave

  • 48.63 eV s-wave

72.30 eV s-wave

5161 keV

(3,4) Details of Entrance Channel

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71 ° 36° 72 ° 108° 90 ° 109° 144°

Downstream

[eV]

lap

E

0.2 0.4 0.6 0.8 1 1.2 1.4

[arbitrary unit]

lap

E ∂ /

γ

I ∂

1 2 3 4 5

= 36 deg

γ

θ [eV]

lap

E

0.2 0.4 0.6 0.8 1 1.2 1.4

[arbitrary unit]

lap

E ∂ /

γ

I ∂

1 2 3 4 5

= 71 deg

γ

θ [eV]

lap

E

0.2 0.4 0.6 0.8 1 1.2 1.4

[arbitrary unit]

lap

E ∂ /

γ

I ∂

1 2 3 4 5

= 72 deg

γ

θ [eV]

lap

E

0.2 0.4 0.6 0.8 1 1.2 1.4

[arbitrary unit]

lap

E ∂ /

γ

I ∂

1 2 3 4 5

= 90 deg

γ

θ [eV]

lap

E

0.2 0.4 0.6 0.8 1 1.2 1.4

[arbitrary unit]

lap

E ∂ /

γ

I ∂

1 2 3 4 5

= 108 deg

γ

θ [eV]

lap

E

0.2 0.4 0.6 0.8 1 1.2 1.4

[arbitrary unit]

lap

E ∂ /

γ

I ∂

1 2 3 4 5

= 144 deg

γ

θ [eV]

lap

E

0.2 0.4 0.6 0.8 1 1.2 1.4

[arbitrary unit]

lap

E ∂ /

γ

I ∂

1 2 3 4 5

= 109 deg

γ

θ

Neutron Energy[eV] Neutron Energy[eV] Neutron Energy[eV] Neutron Energy[eV] Neutron Energy[eV] Neutron Energy[eV] Neutron Energy[eV]

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cos

0.5 − 0.5 0.4 − 0.2 − 0.2

[eV] E

0.2 0.4 0.6 0.8 1 1.2 1.4 1 2 3 4 5

H

Ν

L

Ν

NL NH

Neutron Energy[eV]

ALH = NL − NH NL + NH .

36deg detector

ALH as a function of emission angle

ALH(θγ)=Acosθγ + B A=-0.388±0.024 B=-0.075±0.011

Measured angular dependence Flambaum parametrization

= 0.295 cos φ1 − 0.345 sin φ1.

c c

Comparison with Flambaum’s formalism

(3,4) Details of Entrance Channel

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1 − 0.5 − 0.5 1 0.5 − 0.5 1 − 1

1

φ sin

1

φ cos

22

Okudaira et al., PRC97(2018)034622

κ(J) = 4.84+5.58

−1.69,

0.99+0.08

−0.07

x = −0.16+0.09

−0.11,

−0.95+0.03

−0.04.

= 0.295 cos φ1 − 0.345 sin φ1.

(3,4) Details of Entrance Channel

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page Title(Discrete Symmetry Violation in Neutron-induced Compound States for New Physics Search) Conf(International Workshop for Particle Physics at Neutron Sources (PPNS2018)) Date(2018/05/26) At(Grenoble)

Experimental Apparatus

biological shield p 500MeV spallation moderation

238U

H2O

20Hz ~5µA

superconducting magnet 2.5T beam monitor γ

collimator collimator

Spallation Neutron Source Dynamically Polarized Proton Filter as Neutron Polarizer γ-ray Detectors Neutron Detector

BaF2 10B loaded liquid scintillator

Adiabatic Passage Transmittance Monitor

Ti-sapphire Ar laser Ti-sapphire Ar laser

Adiabatic Passage Adiabatic Passages Superconducting Magnetic Shield

Target Rotatable

Polarized Neutron Source Target station Neutron Spin Analyzer

23

NOPTREX Collaboration KEK 2018S12 Neutron Optics for Parity and Time Reversal EXperiment

epithermal neutron polarizer epithermal neutron spin analyzer polarized target spin control

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page Title(Behavior of Neutron Spin in Polarized Nuclear Target for the T-violation Search in Compound Nuclei) Conf(5th Joint Meeting of the Nuclear Physics Divisions of APS and JPS (HAW2018)) Date(2018/10/27) At(Waikoloa)

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Spin Dependent P-even T-even P-violation P-odd T-even Spin Independent P-even T-even T-violation P-odd T-odd Spin Dependent P-even T-even P-violation P-odd T-even Spin Independent P-even T-even T-violation P-odd T-odd

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page Title(Discrete Symmetry Violation in Neutron-induced Compound States for New Physics Search) Conf(International Workshop for Particle Physics at Neutron Sources (PPNS2018)) Date(2018/05/26) At(Grenoble)

with ultimate polarizations reaches the discovery potential in 45 hours with reported polarizations reaches to the discovery potential in 30 days

1 −

10 1 10

2

10

7 −

10

6 −

10

5 −

10 Graph

Measurement Time [day]

ultimate polarizations reported polarizations

corresponding to dn =3.0×10-26 e cm corresponding to dn =3.0×10-27 e cm

P(3He)=100%, P(139La)=100% P(3He)=70%, P(139La)=40%

25

P(139La)≥0.4, V≥4cm×4cm×6cm B0≤0.1T

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1 − 0.5 − 0.5 1 0.5 − 0.5 1 − 1

1

φ sin

1

φ cos

26

x = −0.16+0.09

−0.11,

−0.95+0.03

−0.04.

= 0.295 cos φ1 − 0.345 sin φ1.

(3,4) Details of Entrance Channel

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P-even T-odd P-odd T-even P-even T-even

Higher-order Tensor Correlation Terms

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f = A0 + B0σ · ˆ I + C0σ · ˆ k + D0σ · (ˆ I × ˆ k)

Spin Independent P-even T-even Spin Dependent P-even T-even P-violation P-odd T-even T-violation P-odd T-odd

Pseudomagnetism

pseudomagnetism

potential scattering compound resonance

V.Gudkov and HMS, Phys. Rev. C95 045501 (2017)

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Polarization Transfer Coefficient

  • 1. freeze target polarization
  • 2. adjust magnetic field to

cancel the pseudomagnetism (Re B’) Alignment, adjustment of experimental apparatus can be measured through the function form of the energy dependence of neutron spin.

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page Title(Discrete Symmetry Violation in Neutron-induced Compound States for New Physics Search) Conf(International Workshop for Particle Physics at Neutron Sources (PPNS2018)) Date(2018/05/26) At(Grenoble)

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The polarized target is the key item. Backup solution

lattice temperature electron spin temperature nuclear spin temperature

DNP: Dynamic Nuclear Polarization

lattice temperature electron spin temperature nuclear spin temperature

Brute-force method

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page Title(Discrete Symmetry Violation in Neutron-induced Compound States for New Physics Search) Conf(International Workshop for Particle Physics at Neutron Sources (PPNS2018)) Date(2018/05/26) At(Grenoble)

31

RCNP Osaka univ.

SPring-8 BL33LEP beamline HD target TC1 DRS SC IBC TC2

HD gas distillation system

SC SC IBC K+ K-

  • Transportation of polarized HD target

18

Brute-force Polarized Target to SPring8 → J-PARC

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Mitchell, Phys. Rep. 354 (2001) 157 Shimizu, Nucl. Phys. A552 (1993) 293

139La 81Br 117Sn 109Ag 238U 232Th 121Sb 131Xe 113Cd 238U 115Rh 133Cs 107Ag 127I 232Th 232Th 111Cd 232Th 232Th 109Ag 113Cd 115In 115In

Survey other target nuclei

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Mitchell, Phys. Rep. 354 (2001) 157 Shimizu, Nucl. Phys. A552 (1993) 293

139La 81Br 117Sn 109Ag 238U 232Th 121Sb 131Xe 113Cd 238U 115Rh 133Cs 107Ag 127I 232Th 232Th 111Cd 232Th 232Th 109Ag 113Cd 115In 115In

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Mitchell, Phys. Rep. 354 (2001) 157 Shimizu, Nucl. Phys. A552 (1993) 293

139La 81Br 117Sn 109Ag 238U 232Th 121Sb 131Xe 113Cd 238U 115Rh 133Cs 107Ag 127I 232Th 232Th 111Cd 232Th 232Th 109Ag 113Cd 115In 115In

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Polarized Target Neutron Spin Filter (n,γ) P-violation Pulsed Epithermal Neutron Beam T-violation Interference

J-PARC LANL J-PARC RCNP RIKEN JAEA KEK JAEA

  • Univ. British Columbia

DNP

SEOP Triplet-DNP

  • Univ. Southern Illinois

Titech, RIKEN IPNS J-PARC E?? 2018S12 Project

“Development of Polarized Target for New Physics Search via T-violation”

IMSS

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NOPTREX Collaboration

W.M.Snow, J.Curole, J.Carini

Indiana University

V.Gudkov

  • Univ. South Carolina

B.Plaster, D.Schaper, C.Crawford

Kentucky Univ.

J.D.Bowman, S.Penttila, X.Tong, P.Jiang

Oak Ridge National Lab.

P.Hautle

Paul Scherrer Institut

A.S.Tremsin

  • Univ. California Berkeley

Southern Illinois University

B.M.Goodson M.Veillette

Berea College

KEK 2018S12 Neutron Optical Parity and Time Reversal EXperiment

H.M.Shimizu, M.Kitaguchi, K.Hirota, T.Yamamoto, K.Ishizaki, S.Endoh, T.Sato, Y.Niinomi, T.Morishima, G.Ichikawa, Y.Kiyanagi, J.Hisano, N,Wada, T.Matsushita T.Yoshioka, S.Takada, J.Koga, S.Makise T.Okudaira, K.Sakai, A.Kimura, H.Harada

Nagoya University Kyushu University JAEA

Y.Yamagata, T.Uesaka, K.Tateishi, H.Ikegami

RIKEN

T.Ino, S.Ishimoto, K.Taketani, K.Mishima, C.C.Haddock

KEK

Y.I.Takahashi, M.Hino

Kyoto Univ.

T.Iwata, Y.Miyachi

Yamagata Univ.

T.Momose

  • Univ. British Columbia

Hiroshima Univ.

M.Iinuma

Osaka Univ.

K.Ogata, H.Kohri, M.Yosoi, T.Shima, H.Yoshikawa

Tohoku Univ.

M.Fujita H.Fujioka

Tokyo Inst. Tech.

D.Takahashi

Ashikaga Univ.

R.Ishiguro

Japan Women’s Univ.

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leading nucleon-level P- and T-odd interaction

nucleon EDM T-odd P-odd pion-nucleon couplings