/*===================================================================*/ /* NRDF D1672 Data No.16 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,16; 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,16; 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,DATA1'44',THTC); /*@44@*/ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,16; INC-ENGY-LAB=6MEV; EMT-1=D; RSD=X; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DATA4'44' DELTA-DATA4 (DEG) (NODIM) (NODIM) 2.104E+01 -1.281E-03 +0.000E+00-0.000E+00 2.400E+01 -1.826E-03 +1.348E-04-3.820E-04 2.703E+01 -3.135E-03 +1.571E-04-2.017E-04 2.975E+01 -3.613E-03 +1.574E-04-2.472E-04 3.353E+01 -3.957E-03 +1.348E-04-2.022E-04 3.729E+01 -4.706E-03 +2.021E-04-4.462E-05 4.015E+01 -6.150E-03 +0.000E+00-0.000E+00 4.367E+01 -7.078E-03 +0.000E+00-0.000E+00 4.711E+01 -8.119E-03 +0.000E+00-0.000E+00 5.029E+01 -9.428E-03 +0.000E+00-0.000E+00 5.251E+01 -1.071E-02 +0.000E+00-0.000E+00 5.564E+01 -1.115E-02 +0.000E+00-4.494E-05 5.853E+01 -1.151E-02 +0.000E+00-0.000E+00 6.307E+01 -1.350E-02 +0.000E+00-0.000E+00 6.731E+01 -1.432E-02 +0.000E+00-0.000E+00 7.179E+01 -1.536E-02 +0.000E+00-0.000E+00 7.452E+01 -1.593E-02 +2.016E-04-3.143E-04 7.930E+01 -1.782E-02 +0.000E+00-0.000E+00 8.280E+01 -1.954E-02 +0.000E+00-0.000E+00 8.631E+01 -2.056E-02 +0.000E+00-0.000E+00 8.909E+01 -2.227E-02 +2.919E-04-3.372E-04 9.133E+01 -2.261E-02 +0.000E+00-3.222E-07 9.274E+01 -2.407E-02 +3.593E-04-2.249E-04 9.691E+01 -2.473E-02 +4.937E-04-4.266E-04 1.012E+02 -2.638E-02 +1.794E-04-2.698E-04 1.064E+02 -2.911E-02 +1.573E-04-2.249E-04 1.107E+02 -2.984E-02 +5.845E-04-1.565E-04 1.138E+02 -3.016E-02 +2.252E-04-4.044E-04 1.172E+02 -2.943E-02 +2.700E-04-3.823E-04 1.215E+02 -2.811E-02 +2.021E-04-1.574E-04 1.257E+02 -2.720E-02 +0.000E+00-0.000E+00 1.272E+02 -2.551E-02 +2.695E-04-4.264E-04 1.294E+02 -2.460E-02 +3.590E-04-3.815E-04 1.318E+02 -2.316E-02 +3.364E-04-4.714E-04 1.344E+02 -2.213E-02 +3.375E-04-3.370E-04 1.357E+02 -2.038E-02 +0.000E+00-0.000E+00 1.387E+02 -1.918E-02 +0.000E+00-0.000E+00 1.407E+02 -1.736E-02 +2.465E-04-3.372E-04 1.431E+02 -1.582E-02 +2.017E-04-2.693E-04 1.450E+02 -1.407E-02 +0.000E+00-0.000E+00 1.465E+02 -1.331E-02 +0.000E+00-0.000E+00 1.485E+02 -1.133E-02 +2.918E-04-4.489E-04 1.503E+02 -1.057E-02 +3.142E-04-3.592E-04 1.528E+02 -9.341E-03 +0.000E+00-0.000E+00 1.532E+02 -6.848E-03 +2.472E-04-2.473E-04 1.556E+02 -6.223E-03 +1.566E-04-2.924E-04 1.578E+02 -5.014E-03 +2.467E-04-3.597E-04 1.597E+02 -4.434E-03 +2.008E-04-3.369E-04 1.623E+02 -3.743E-03 +3.602E-04-2.017E-04 1.639E+02 -1.633E-03 +2.468E-04-2.019E-04 1.673E+02 -2.090E-03 +1.793E-04-4.707E-04 \END; /*===================================================================*/ |