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Tensor Analyzing Powers of pd Radiative Capture

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Tensor Analyzing Powers of pd Radiative Capture. Y. Tameshige , K. Sagara a , T. Kudoh a , M.Shiota a , S. Shimomoto a , T.Wakasa a , K. Hatanaka, A. Tamii, Y. Sakemi, Y. Shimizu, H.P.Yoshida a , H.Kamada b , and H. Wita l a c RCNP Osaka University, - PowerPoint PPT Presentation
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Tensor Analyzing Powers of pd Radiative Capture Y. Tameshige , K. Sagara a , T. Kudoh a , M.Shi ota a , S. Shimomoto a , T.Wakasa a , K. Hatanaka, A. Tamii, Y. Sakemi, Y. Shim izu, H.P.Yoshida a , H.Kamada b , and H. Witala c RCNP Osaka University, a Department of Physics, Kyushu University b Faculty of Engineering, Kyushu Institute of Technology c Department of Physics, Yagellonian Unive rsity
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Page 1: Tensor Analyzing Powers of  pd  Radiative Capture

Tensor Analyzing Powers of pd Radiative Capture

Y. Tameshige, K. Sagaraa, T. Kudoha, M.Shiotaa, S. Shimomotoa, T.Wakasaa,

K. Hatanaka, A. Tamii, Y. Sakemi, Y. Shimizu, H.P.Yoshidaa,

H.Kamadab, and H. Witalac

RCNP Osaka University, aDepartment of Physics, Kyushu University

bFaculty of Engineering, Kyushu Institute of TechnologycDepartment of Physics, Yagellonian University

Page 2: Tensor Analyzing Powers of  pd  Radiative Capture

contents

• Introduction

• Experiment

• Results

• Summary &Future Plan

Page 3: Tensor Analyzing Powers of  pd  Radiative Capture

Introduction

N N N

CD Bonn

AV18

Nijm93

Ruhr

8.00

7.65

7.66

7.64

8.483

8.479

8.480

8.459

4.86

5.22

5.10

5.31

NN pot. NN only NN+3NF(TM) (m)

Exp. 8.48 MeV3H biding energy

N N N

Higher-order 3NF (short range)

N N N

However, even if 23NF is included,

polarization observables of pd scattering

can not be reproduced.

Higher-order 3NF may be necessary.

Page 4: Tensor Analyzing Powers of  pd  Radiative Capture

Axz

Ed=

140MeV

Ed=

200MeV

Ed=

270MeV

Ayd Ayy

K. Sekiguchi et al.

Axx

NN NN+3NF

Adding a 3NF does not improve the description of the data.

indicating deficiencies in the spin-dependent part of present 3NF models

Page 5: Tensor Analyzing Powers of  pd  Radiative Capture

pd capture reaction may be a probe of short range forces.

N N N

Higher-order 3NF (short range)

N N N

However, even if 23NF is included,

polarization observables of pd scattering

can not be reproduced.

Higher-order 3NF may be necessary.

Discrepancies in polarization observables

of pd scattering are complicated.

Simple and clear signatures are required to

study higher-order 3NF.

+ +

Candidate to find out short distance three nucleon reaction

Page 6: Tensor Analyzing Powers of  pd  Radiative Capture

Present study: pd capture experiment

+ +

In pd capture reaction,

○  Short-range forces may play important roles. (→short range

3NF)

×   Reaction cross section is very small (~ 0.1 barn).

Experimental techniques•thick target & low BG   →  liquid hydrogen target •high-efficiency detection → one-shot measurement of whole

                     angular distribution

Page 7: Tensor Analyzing Powers of  pd  Radiative Capture

p+d →3He+γ experiment at Ed = 137 MeV

Ayy (pure tensor)

(Pyy = -1.2)

Axx (pure tensor)

Experimental setup

1.5mm(10mg/cm2)

Ed = 137 MeV(4nA)

Page 8: Tensor Analyzing Powers of  pd  Radiative Capture

Vertical planefor Axx

Horizontal planefor Ayy

d + p→3He+(3He) < 4.1

Angular distribution in 20~160 was taken in one shot.

d-beam isvertically polarized

2°3°

4°5°Axx

Axx

FC shadow

Slit in front of LAS

Ayy

2° 3° 4° 5°

LAS acceptance horizontally ±3.4 [deg] ( ±60 [mrad])

vertically ±5.7 [deg] (±100 [mrad])

LAS at 2.5°LAS at 0°

Φ20

Page 9: Tensor Analyzing Powers of  pd  Radiative Capture

Liquid Hydrogen TargetExperimental setup

Page 10: Tensor Analyzing Powers of  pd  Radiative Capture

Data analysis

Raw data from liquid H2 target(normal target)

Backgroundsfrom windows(empty target)

X vs Y X vs θ

θcm=0°θcm=180°

θcm=20°

θcm=170°

Axx (0°) Ayy (2.5°)

Page 11: Tensor Analyzing Powers of  pd  Radiative Capture

Data analysis of Axx

projection

projection

Liquid Hydrogen target(normal target)Aramid foil target(empty target)

θcm=180°θcm=0°

X [mm]

Y [m

m]

180°

Page 12: Tensor Analyzing Powers of  pd  Radiative Capture

Data analysis of Ayy

projection

θcm=20°

θcm=170°

Liquid Hydrogen target(normal target)Aramid foil target(empty target)

The same beam charge is the same background tail.

Page 13: Tensor Analyzing Powers of  pd  Radiative Capture

ExperimentalResults

Page 14: Tensor Analyzing Powers of  pd  Radiative Capture

Result at137MeV

present dataAV18AV18+URBIX

●- - -

AyyAxx

Calc. byKamada et al.

Measured Axx largely disagrees with calculations, and 2p3NF can not explain the difference

Page 15: Tensor Analyzing Powers of  pd  Radiative Capture

Ayy

137MeV

196MeV

Axx Axx

Axx

Page 16: Tensor Analyzing Powers of  pd  Radiative Capture

Axx & Ayy at 137MeV

Axx

Ayy

AV18 AV18+URBIX

●●

- - -―

Page 17: Tensor Analyzing Powers of  pd  Radiative Capture

Ayy AzzAxx

・  Axx ~ Ayy means the reaction is z-axial symmetry.

x

y

beam

・  Axx ~ Ayy <0 and Azz>0 means the reaction is dominant in the central region.

Page 18: Tensor Analyzing Powers of  pd  Radiative Capture

RCNP(137MeV) and at 133 MeV (KVI)AyyAxx

present dataKVI dataAV18AV18+URBIX

● (●)●

- - -―

(PRB617,2005,18) at 133MeV

・ The disagreement also exist at 196MeV(RCNP) and 188MeV(KVI) data.

・ We plan to measurements Azz at 196MeV to check the consistency our data.

Page 19: Tensor Analyzing Powers of  pd  Radiative Capture

・ Present data confirmed the Axx~Ayy relation and the large discrepancy in Axx. ・ Present data at 137MeV and 196MeV data show smooth energy dependence.

KVIA xx

Ayy

AyyAxx

Ayy & Axx measured

Only Ayy measured

Present data RCNP

Energy dependence of Axx (90) and Ayy (90)

Page 20: Tensor Analyzing Powers of  pd  Radiative Capture

Summary

・ Axx and Ayy of pd-capture reaction at Ed=137,196 MeV were measured. ・ Measured Axx largely disagrees with calculations, and 23NF can not explain the difference.

・ Data shows Axx ~ Ayy whereas Axx≠Ayy in calculation. The relation Axx ~ Ayy may be a possible signature of short-range force (3NF).

・ RCNP data and KVI data disagree in the absolute values.

A new experiment on Azz at 196 MeV

will be made in October 2006 (5days later).

Page 21: Tensor Analyzing Powers of  pd  Radiative Capture

Present data at 137MeVKVI dataAV18AV18+URBIX

●●

- - -―

(PRB617,2005,18) at 133MeV

Axx at RCNP(137MeV) and at 133 MeV (KVI)

Page 22: Tensor Analyzing Powers of  pd  Radiative Capture

present dataKVI dataAV18AV18+URBIX

●●

- - -―

Ayy at RCNP(137MeV) and at 133 MeV (KVI)

(PRB617,2005,18) at 133MeV


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