/*===================================================================*/ /* 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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