DARPE: Search Results
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 /* NRDF D1807 Data No.2                                              */
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 /* Bibliography                                                      */
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 \\BIB,2;
 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 */
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 /* Experimental Conditions                                           */
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 \\EXP,2;
 /* 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=POL-TRNSF'20';
 /* '20' Total spin transfer multiplied by double differential
         cross section */
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
 INC-ENGY-LAB=392MEV;
 THTL=0[1DEG;
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 /* Data Table                                                        */
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 \DATA;
 EXC-ENGY DATA1'21' DELTA-DATA1'21,22'
 (MEV) (MB/SR/MEV) (MB/SR/MEV)
 7.500e+00 5.840e-03 +-3.164e-03
 7.700e+00 -1.844e-02 +-4.790e-02
 7.900e+00 1.759e-02 +-3.254e-02
 8.100e+00 3.184e-02 +-1.904e-02
 8.700e+00 -4.056e-03 +-2.647e-02
 8.900e+00 3.719e-02 +-2.704e-02
 9.100e+00 5.050e-02 +-2.252e-02
 9.300e+00 -2.658e-02 +-2.361e-02
 9.500e+00 2.431e-02 +-2.644e-02
 9.700e+00 -3.531e-03 +-2.529e-02
 9.900e+00 7.195e-02 +-2.503e-02
 1.010e+01 -3.237e-02 +-2.580e-02
 1.030e+01 -3.506e-02 +-2.290e-02
 1.050e+01 3.261e-02 +-2.530e-02
 1.070e+01 2.746e-02 +-2.283e-02
 1.090e+01 -1.050e-03 +-2.434e-02
 1.110e+01 3.368e-02 +-2.341e-02
 1.130e+01 -5.700e-03 +-2.501e-02
 1.150e+01 -6.195e-04 +-2.837e-02
 1.170e+01 5.225e-02 +-2.783e-02
 1.190e+01 1.321e-02 +-3.111e-02
 1.270e+01 4.199e-01 +-3.358e-02
 1.290e+01 8.145e-01 +-4.298e-02
 1.310e+01 7.365e-02 +-1.705e-02
 1.330e+01 3.780e-02 +-2.563e-02
 1.350e+01 1.231e-02 +-1.922e-02
 1.370e+01 1.999e-02 +-2.277e-02
 1.390e+01 1.677e-02 +-2.155e-02
 1.410e+01 5.850e-02 +-2.281e-02
 1.430e+01 1.061e-02 +-1.896e-02
 1.450e+01 4.607e-04 +-1.720e-02
 1.470e+01 4.189e-02 +-1.690e-02
 1.490e+01 5.348e-02 +-1.620e-02
 1.510e+01 6.988e+00 +-8.932e-02
 1.530e+01 7.828e+00 +-8.832e-02
 1.550e+01 3.241e-01 +-1.787e-02
 1.570e+01 9.205e-02 +-1.574e-02
 1.590e+01 2.431e-02 +-1.832e-02
 1.610e+01 1.394e-01 +-2.207e-02
 1.630e+01 1.007e-01 +-1.912e-02
 1.650e+01 5.930e-02 +-2.130e-02
 1.670e+01 5.635e-02 +-1.937e-02
 1.690e+01 1.131e-02 +-1.910e-02
 1.710e+01 7.985e-02 +-2.035e-02
 1.730e+01 5.060e-02 +-1.767e-02
 1.750e+01 8.325e-02 +-2.191e-02
 1.770e+01 4.987e-02 +-2.204e-02
 1.790e+01 1.000e-01 +-2.229e-02
 1.810e+01 2.954e-01 +-2.671e-02
 1.830e+01 4.495e-01 +-3.063e-02
 1.850e+01 3.832e-01 +-2.859e-02
 1.870e+01 2.147e-01 +-2.705e-02
 1.890e+01 2.374e-01 +-2.959e-02
 1.910e+01 4.735e-01 +-3.499e-02
 1.930e+01 8.275e-01 +-4.031e-02
 1.950e+01 1.054e+00 +-4.182e-02
 1.970e+01 7.690e-01 +-3.567e-02
 1.990e+01 6.880e-01 +-3.537e-02
 2.010e+01 4.292e-01 +-3.177e-02
 2.030e+01 3.133e-01 +-3.044e-02
 2.050e+01 2.724e-01 +-2.902e-02
 2.070e+01 2.465e-01 +-2.771e-02
 2.090e+01 2.681e-01 +-2.736e-02
 2.110e+01 2.758e-01 +-2.870e-02
 2.130e+01 2.344e-01 +-2.916e-02
 2.150e+01 2.671e-01 +-3.064e-02
 2.170e+01 3.547e-01 +-3.259e-02
 2.190e+01 4.425e-01 +-3.392e-02
 2.210e+01 4.460e-01 +-3.331e-02
 2.230e+01 3.994e-01 +-3.265e-02
 2.250e+01 4.680e-01 +-3.268e-02
 2.270e+01 4.184e-01 +-3.292e-02
 2.290e+01 4.222e-01 +-3.152e-02
 2.310e+01 3.187e-01 +-3.096e-02
 2.330e+01 2.747e-01 +-2.942e-02
 2.350e+01 2.545e-01 +-2.789e-02
 2.370e+01 2.530e-01 +-2.763e-02
 2.390e+01 2.497e-01 +-2.701e-02
 2.410e+01 2.290e-01 +-2.502e-02
 2.430e+01 2.164e-01 +-2.547e-02
 2.450e+01 1.863e-01 +-2.335e-02
 2.470e+01 1.805e-01 +-2.385e-02
 2.490e+01 1.941e-01 +-2.434e-02
 2.510e+01 2.074e-01 +-2.649e-02
 2.530e+01 2.385e-01 +-2.680e-02
 2.550e+01 2.475e-01 +-2.673e-02
 2.570e+01 3.044e-01 +-2.648e-02
 2.590e+01 1.755e-01 +-2.446e-02
 2.610e+01 2.021e-01 +-2.414e-02
 2.630e+01 2.121e-01 +-2.355e-02
 2.650e+01 1.574e-01 +-2.290e-02
 2.670e+01 1.954e-01 +-2.279e-02
 2.690e+01 1.781e-01 +-2.228e-02
 2.710e+01 1.855e-01 +-2.351e-02
 2.730e+01 1.598e-01 +-2.133e-02
 2.750e+01 2.263e-01 +-2.396e-02
 2.770e+01 1.865e-01 +-2.308e-02
 2.790e+01 1.683e-01 +-2.418e-02
 2.810e+01 1.752e-01 +-2.491e-02
 2.830e+01 1.995e-01 +-2.298e-02
 2.850e+01 1.925e-01 +-2.284e-02
 2.870e+01 1.900e-01 +-2.203e-02
 2.890e+01 1.320e-01 +-2.207e-02
 2.910e+01 1.986e-01 +-2.157e-02
 2.930e+01 1.620e-01 +-2.099e-02
 2.950e+01 1.779e-01 +-2.230e-02
 2.970e+01 1.613e-01 +-2.022e-02
 2.990e+01 1.190e-01 +-1.948e-02
 3.010e+01 1.513e-01 +-2.190e-02
 3.030e+01 1.263e-01 +-2.205e-02
 3.050e+01 1.147e-01 +-2.150e-02
 3.070e+01 1.366e-01 +-2.097e-02
 3.090e+01 1.240e-01 +-2.087e-02
 3.110e+01 1.664e-01 +-2.142e-02
 3.130e+01 1.591e-01 +-2.161e-02
 3.150e+01 1.273e-01 +-2.021e-02
 3.170e+01 1.093e-01 +-1.977e-02
 3.190e+01 1.212e-01 +-2.178e-02
 3.210e+01 1.503e-01 +-1.969e-02
 3.230e+01 1.409e-01 +-2.195e-02
 3.250e+01 1.208e-01 +-2.293e-02
 3.270e+01 1.691e-01 +-2.294e-02
 3.290e+01 1.332e-01 +-2.162e-02
 3.310e+01 1.175e-01 +-1.943e-02
 3.330e+01 1.183e-01 +-2.152e-02
 3.350e+01 1.272e-01 +-2.244e-02
 \END;
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