/*===================================================================*/ /* NRDF D1672 Data No.10 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,10; D#=D1672; TITLE=/ANALYSING POWERS OF P+D SCATTERING BELOW THE DEUTERON BREAKUP THRESHOLD/; ATH=(S.SHIMIZU'1',K.SAGARA'1',H.NAKAMURA'1',K.MAEDA'1',T.MIWA'1', N.NISHIMORI'1',S.UENO'1',T.NAKASHIMA'1',S.MORINOBU'1'); INST-ATH=(2JPNKYU'1'); REF=PR/C; VLP=52(1995)1193; RCTS=(D(P,P)X,P(D,D)X); PHQS=(ANALPW,TNSR-ANALPW,ANGL-DSTRN, DATA1'41',DATA2'42',DATA3'43',DATA4'44'); /*@41@*/ /*@42@*/ /*@43@*/ /*@44@*/ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,10; RCT=P(D,D)X; RTY=(POL-RCT); ENR=NAT; CHM=ELM; PHYS-FORM=GAS; THK-TGT=0.27ATM; BAC=SELF; POL-TGT=0.70%; ACC=(VDGT); INST-ACC=2JPNKYU; INC-ENGY-LAB=(2,2.5,3,4,5,6MEV); DET-PARTCL=(D); COINC=NO; ANT-COINC=NO; DET-SYS=(SSD); SOLID-ANGL=XMSR; ERS-DET=XKEV; MONTR-RCT=/@THE POLARIZATION OF THE BEAM WAS MEASURED THROUGHOUT THE EXPERIMENT BY A P+4HE POLAEIMETER PLACED AT THE DOWNSTREAM WND OF THE SCATTERING CHAMBER.@/; ANL=X'45'; /*@45@*/ PHQ=TNSR-ANALPW'41'; /*@41@*/ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,10; INC-ENGY-LAB=6MEV; EMT-1=D; RSD=X; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DATA1'41' DELTA-DATA1 (DEG) (NODIM) (NODIM) 2.182E+01 4.214E-03 +3.613E-04-6.643E-05 2.479E+01 4.962E-03 +1.612E-04-1.336E-04 2.740E+01 5.511E-03 +2.830E-04-1.458E-04 3.006E+01 5.886E-03 +2.807E-04-1.875E-04 3.301E+01 6.112E-03 +2.150E-04-2.146E-04 3.602E+01 6.151E-03 +2.146E-04-1.065E-04 3.956E+01 6.909E-03 +1.081E-04-2.952E-04 4.269E+01 7.670E-03 +3.455E-04-2.292E-04 4.790E+01 7.832E-03 +3.876E-04-3.164E-04 5.053E+01 8.474E-03 +1.989E-04-2.811E-04 5.435E+01 9.004E-03 +1.765E-04-2.123E-04 5.699E+01 9.687E-03 +1.745E-04-2.280E-04 5.996E+01 1.090E-02 +1.478E-04-2.009E-04 6.351E+01 1.127E-02 +1.741E-04-1.333E-04 6.618E+01 1.170E-02 +1.616E-04-2.280E-04 7.063E+01 1.302E-02 +1.482E-04-1.875E-04 7.459E+01 1.431E-02 +1.340E-04-2.390E-04 7.835E+01 1.631E-02 +1.592E-04-1.344E-04 8.370E+01 1.721E-02 +1.608E-04-1.741E-04 8.835E+01 1.965E-02 +1.600E-04-2.009E-04 9.050E+01 2.081E-02 +2.936E-04-5.232E-04 9.209E+01 2.157E-02 +0.000E+00-0.000E+00 9.403E+01 2.284E-02 +4.135E-04-4.658E-04 9.749E+01 2.364E-02 +4.576E-04-5.338E-04 1.011E+02 2.564E-02 +3.349E-04-3.750E-04 1.054E+02 2.553E-02 +3.499E-04-4.544E-04 1.096E+02 2.630E-02 +3.994E-04-3.900E-04 1.140E+02 2.581E-02 +4.277E-04-5.452E-04 1.181E+02 2.484E-02 +3.616E-04-4.269E-04 1.221E+02 2.459E-02 +2.146E-04-1.620E-04 1.259E+02 2.178E-02 +2.669E-04-7.979E-05 1.277E+02 2.063E-02 +1.616E-04-1.470E-04 1.293E+02 1.876E-02 +3.094E-04-5.601E-04 1.312E+02 1.767E-02 +3.605E-04-6.022E-04 1.326E+02 1.646E-02 +4.815E-04-5.452E-04 1.347E+02 1.619E-02 +1.352E-04-8.019E-05 1.368E+02 1.462E-02 +3.337E-04-5.436E-04 1.388E+02 1.450E-02 +4.305E-04-4.171E-04 1.412E+02 1.282E-02 +3.074E-04-2.304E-04 1.436E+02 1.175E-02 +1.745E-04-2.539E-04 1.456E+02 1.075E-02 +2.017E-04-2.009E-04 1.478E+02 1.010E-02 +1.887E-04-3.994E-04 1.500E+02 9.993E-03 +3.078E-04-3.746E-04 1.524E+02 7.747E-03 +2.029E-04-2.819E-04 1.534E+02 7.769E-03 +2.005E-04-3.078E-04 1.553E+02 7.599E-03 +2.005E-04-3.475E-04 1.571E+02 6.253E-03 +4.289E-04-3.754E-04 1.585E+02 6.192E-03 +2.653E-04-2.523E-04 1.604E+02 5.099E-03 +4.135E-04-4.006E-04 1.622E+02 3.298E-03 +3.601E-04-3.070E-04 1.649E+02 4.101E-03 +4.815E-04-3.212E-04 \END; /*===================================================================*/ |