|
| /*===================================================================*/
/* NRDF D1807 Data No.3 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,3;
D#=D1807;
TITLE=/ Polarization transfer observables for proton inelastic
scattering from 12C at 0 degree /;
PURPOSE=/ To study the effective interaction of nucleon-nucleus
scattering in intermediate energy /;
ATH=(A.TAMII'1', H.AKIMUNE'2', I.DAITO'3', Y.FUJITA'4', M.FUJIWARA'2,
5', K.HATANAKA'5', K.HOSONO'6', F.IHARA'5', T.INOMATA'5',
T.ISHIKAWA'7', M.ITOH'7', M.KAWABATA'8', T.KAWABATA'7',
M.NAKAMURA'7', T.NORO'5', E.OBAYASHI'5', H.SAKAGUCHI'7',
H.TAKEDA'7', T.TAKI'7', H.TOYOKAWA'9', H.P.YOSHIDA'5',
M.YOSHIMURA'5', M.YOSOI'7');
INST-ATH=(2JPNTOK'1', 2JPNJAE'2', 2JPNNAG'3', 2JPNOSA'4', 2JPNRCN'5',
2JPNHIT'6', 2JPNKTO'7', 2JPNTOH'8', 2JPNJSR'9');
/* '1' Department of Physics */
/* '2' Advanced Science Research Center */
/* '3' Center for Integrated Research in Science and Engineering
/* '4' Department of Physics */
/* '6' Department of Engineering */
/* '7' Department of Physics */
/* '8' Laboratory of Nuclear Science */
REF=PL/B;
VLP=459(1999)61;
/* Secondary reference
- Tamii, Thesis(1999)
RCTS=12C(P,P)12C;
PHQS=(ENGY-SPEC, POL-TRNSF'10', SFLP'11', POL-TRNSF'12',
POL-TRNSF'13', POL-TRNSF'14', ANGL-DSTRN, POL-TRNSF);
/* '10' Total spin transfer multiplied by double differential cross
section */
/* '11' double differential cross section multiplied by
(longitudinal spin-flip probability S(L'L)-transverse spin-flip
probability S(S'S)) */
/* '12' D(SS) */
/* '13' D(LL) */
/* '14' Total spin transfer */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,3;
/* 2003-07-15 : Compiled, Im + Ia */
ENR=NAT;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=30MG/CM**2;
BAC=SELF;
ALGN-TGT=0%;
ACC=CYC;
INST-ACC=2JPNRCN;
INC-ENGY-LAB=392MEV;
BEAM-INTNSTY=2[3NA;
POL-PRJ=[75%'15';
/* '15' Monitored by two sets of beam-line polarimeters with a
polystyrene sheet as the analyzer target. */
DET-PARTCL=P;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG'16',MWDC'17',MWPC'18');
/* '16' Grand Raiden [M. Fujiwara, Nucl. Instr. Meth. in Phys.
Res. A 422(1999)484] */
/* '17' To detect the position and incidence angle of scattered
protons at the focal plane */
/* '18' Focal Plane Polarimeter (FPP) system [M. Yosoi et al.,
in: K.J. Heller, S.L. Smith Eds. , Proc. 11th Int. Symp. on
High Energy Spin Physics, AIP Conf. Proc. No. 343, AIP, New
York, 1995, p. 157] consisted of four MWPC and a PS hodoscope
in Grand Raiden. To measure polarization of protons */
ERS-DET=120KEV;
/* Experimental Method:
- Ray-tracking technique to get scattering angle
- Double scattering (To measure the polarization of scattered
proton)
RCT=12C(P,P)12C;
RTY=(INEL-SCATT,POL-RCT);
PHQ=SFLP'23';
/* '23' double differential cross section multiplied by
(longitudinal spin-flip probability S(L'L)-transverse
spin-flip probability S(S'S)) */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,3;
INC-ENGY-LAB=392MEV;
THTL=0[1DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY DATA1'24' DELTA-DATA1'24,25'
(MEV) (MB/SR/MEV) (MB/SR/MEV)
7.500e+00 -5.875e-03 +-5.680e-03
7.700e+00 -3.042e-02 +-6.005e-02
7.900e+00 4.344e-02 +-4.189e-02
8.100e+00 -5.175e-02 +-2.058e-02
8.700e+00 5.835e-02 +-3.224e-02
8.900e+00 -1.167e-02 +-3.338e-02
9.100e+00 -3.194e-02 +-2.780e-02
9.300e+00 7.510e-03 +-2.967e-02
9.500e+00 -1.318e-02 +-3.278e-02
9.700e+00 2.447e-02 +-3.144e-02
9.900e+00 -5.095e-02 +-3.116e-02
1.010e+01 1.760e-02 +-3.228e-02
1.030e+01 5.150e-02 +-2.892e-02
1.050e+01 -4.985e-02 +-3.196e-02
1.070e+01 -1.440e-02 +-2.910e-02
1.090e+01 8.070e-03 +-3.090e-02
1.110e+01 -3.666e-02 +-2.990e-02
1.130e+01 2.114e-02 +-3.115e-02
1.150e+01 -2.261e-02 +-3.605e-02
1.170e+01 -1.334e-02 +-3.314e-02
1.190e+01 -6.245e-03 +-3.883e-02
1.270e+01 -3.566e-01 +-4.129e-02
1.290e+01 -6.295e-01 +-5.600e-02
1.310e+01 -4.004e-02 +-2.146e-02
1.330e+01 1.211e-02 +-3.111e-02
1.350e+01 1.125e-02 +-2.349e-02
1.370e+01 6.140e-03 +-2.711e-02
1.390e+01 8.115e-03 +-2.695e-02
1.410e+01 1.002e-03 +-2.854e-02
1.430e+01 -1.264e-02 +-2.508e-02
1.450e+01 -4.344e-03 +-2.212e-02
1.470e+01 1.416e-02 +-2.117e-02
1.490e+01 1.376e-02 +-1.795e-02
1.510e+01 9.040e-01 +-1.008e-01
1.530e+01 2.053e+00 +-1.048e-01
1.550e+01 1.221e-01 +-2.280e-02
1.570e+01 3.048e-02 +-1.932e-02
1.590e+01 4.629e-02 +-2.292e-02
1.610e+01 4.747e-02 +-2.737e-02
1.630e+01 5.705e-02 +-2.461e-02
1.650e+01 2.264e-02 +-2.756e-02
1.670e+01 -1.172e-02 +-2.474e-02
1.690e+01 6.975e-03 +-2.482e-02
1.710e+01 2.292e-02 +-2.651e-02
1.730e+01 -4.490e-03 +-2.295e-02
1.750e+01 3.129e-02 +-2.835e-02
1.770e+01 1.474e-02 +-2.861e-02
1.790e+01 -7.405e-02 +-2.854e-02
1.810e+01 -1.743e-01 +-3.315e-02
1.830e+01 -3.588e-01 +-3.841e-02
1.850e+01 -2.508e-01 +-3.620e-02
1.870e+01 -8.770e-02 +-3.499e-02
1.890e+01 1.269e-02 +-3.741e-02
1.910e+01 7.035e-03 +-4.329e-02
1.930e+01 4.729e-02 +-4.980e-02
1.950e+01 8.590e-02 +-5.170e-02
1.970e+01 9.115e-02 +-4.389e-02
1.990e+01 -2.092e-02 +-4.375e-02
2.010e+01 5.235e-02 +-4.056e-02
2.030e+01 -5.350e-02 +-3.839e-02
2.050e+01 -5.630e-02 +-3.723e-02
2.070e+01 -7.795e-02 +-3.536e-02
2.090e+01 -1.563e-02 +-3.524e-02
2.110e+01 -2.781e-02 +-3.638e-02
2.130e+01 3.121e-02 +-3.771e-02
2.150e+01 8.160e-02 +-3.909e-02
2.170e+01 1.069e-01 +-4.176e-02
2.190e+01 4.781e-02 +-4.306e-02
2.210e+01 7.390e-02 +-4.251e-02
2.230e+01 5.510e-03 +-4.251e-02
2.250e+01 4.554e-02 +-4.197e-02
2.270e+01 7.660e-02 +-4.242e-02
2.290e+01 6.465e-02 +-4.056e-02
2.310e+01 5.840e-02 +-3.964e-02
2.330e+01 1.770e-02 +-3.818e-02
2.350e+01 -1.775e-02 +-3.603e-02
2.370e+01 2.149e-02 +-3.576e-02
2.390e+01 -3.289e-02 +-3.530e-02
2.410e+01 9.260e-03 +-3.279e-02
2.430e+01 -1.898e-02 +-3.318e-02
2.450e+01 3.280e-02 +-3.073e-02
2.470e+01 -1.019e-02 +-3.103e-02
2.490e+01 1.523e-02 +-3.148e-02
2.510e+01 -4.335e-02 +-3.426e-02
2.530e+01 -9.615e-03 +-3.443e-02
2.550e+01 -6.800e-03 +-3.449e-02
2.570e+01 -3.784e-02 +-3.392e-02
2.590e+01 4.102e-02 +-3.202e-02
2.610e+01 5.830e-03 +-3.138e-02
2.630e+01 -8.095e-02 +-3.047e-02
2.650e+01 7.875e-02 +-2.978e-02
2.670e+01 -1.211e-02 +-2.905e-02
2.690e+01 -3.157e-03 +-2.825e-02
2.710e+01 -2.123e-03 +-3.045e-02
2.730e+01 4.637e-02 +-2.722e-02
2.750e+01 3.372e-02 +-3.078e-02
2.770e+01 -8.585e-04 +-2.939e-02
2.790e+01 -3.526e-02 +-3.097e-02
2.810e+01 -3.501e-02 +-3.229e-02
2.830e+01 -4.860e-02 +-2.965e-02
2.850e+01 -1.820e-02 +-2.950e-02
2.870e+01 -9.870e-03 +-2.840e-02
2.890e+01 -2.834e-03 +-2.870e-02
2.910e+01 -5.595e-03 +-2.772e-02
2.930e+01 9.870e-03 +-2.697e-02
2.950e+01 4.899e-03 +-2.889e-02
2.970e+01 3.830e-02 +-2.612e-02
2.990e+01 -4.999e-02 +-2.609e-02
3.010e+01 -2.037e-02 +-2.830e-02
3.030e+01 -3.967e-02 +-2.862e-02
3.050e+01 -7.245e-04 +-2.861e-02
3.070e+01 3.560e-02 +-2.772e-02
3.090e+01 -1.732e-02 +-2.763e-02
3.110e+01 -2.858e-03 +-2.756e-02
3.130e+01 -7.065e-03 +-2.818e-02
3.150e+01 1.059e-02 +-2.665e-02
3.170e+01 1.217e-03 +-2.585e-02
3.190e+01 2.115e-02 +-2.946e-02
3.210e+01 1.561e-02 +-2.599e-02
3.230e+01 5.760e-02 +-2.946e-02
3.250e+01 4.072e-02 +-2.972e-02
3.270e+01 5.235e-02 +-3.004e-02
3.290e+01 -3.083e-02 +-2.820e-02
3.310e+01 -6.580e-03 +-2.552e-02
3.330e+01 4.475e-02 +-2.839e-02
3.350e+01 -2.631e-02 +-3.040e-02
\END;
/*===================================================================*/
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