/*===================================================================*/ /* NRDF D1672 Data No.1 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,1; 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,1; RCT=D(P,P)X; RTY=(POL-RCT); ENR=NAT; CHM=ELM; PHYS-FORM=GAS; THK-TGT=0.27ATM; BAC=SELF; POL-TGT=X%'22'; /*@22@*/ ACC=(VDGT); INST-ACC=2JPNKYU; INC-ENGY-LAB=(2,2.5,3,4,5,6MEV); DET-PARTCL=(P); 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=(ANGL-DSTRN,THTC); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,1; INC-ENGY-LAB=2.5MEV; EMT-1=P; RSD=X; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 2.193E+01 3.798E+02 +5.002E+00-3.732E+00 2.444E+01 3.111E+02 +2.136E+00-3.554E+00 2.725E+01 2.704E+02 +1.964E+00-3.373E+00 2.929E+01 2.425E+02 +0.000E+00-0.000E+00 3.199E+01 2.292E+02 +0.000E+00-0.000E+00 3.501E+01 2.175E+02 +0.000E+00-0.000E+00 3.833E+01 2.092E+02 +0.000E+00-0.000E+00 4.102E+01 2.009E+02 +0.000E+00-0.000E+00 4.434E+01 1.945E+02 +0.000E+00-0.000E+00 4.742E+01 1.862E+02 +0.000E+00-0.000E+00 4.993E+01 1.806E+02 +0.000E+00-0.000E+00 5.286E+01 1.728E+02 +0.000E+00-0.000E+00 5.521E+01 1.664E+02 +0.000E+00-0.000E+00 5.756E+01 1.608E+02 +0.000E+00-0.000E+00 6.000E+01 1.539E+02 +0.000E+00-0.000E+00 6.235E+01 1.477E+02 +0.000E+00-0.000E+00 6.494E+01 1.431E+02 +0.000E+00-0.000E+00 6.786E+01 1.367E+02 +0.000E+00-0.000E+00 7.077E+01 1.322E+02 +0.000E+00-0.000E+00 7.674E+01 1.252E+02 +0.000E+00-0.000E+00 8.094E+01 1.197E+02 +0.000E+00-0.000E+00 8.458E+01 1.144E+02 +0.000E+00-0.000E+00 8.789E+01 1.102E+02 +0.000E+00-0.000E+00 9.127E+01 1.080E+02 +0.000E+00-0.000E+00 9.482E+01 1.065E+02 +0.000E+00-0.000E+00 9.891E+01 1.076E+02 +0.000E+00-0.000E+00 1.034E+02 1.102E+02 +0.000E+00-0.000E+00 1.084E+02 1.172E+02 +0.000E+00-0.000E+00 1.127E+02 1.244E+02 +0.000E+00-0.000E+00 1.156E+02 1.346E+02 +0.000E+00-0.000E+00 1.183E+02 1.466E+02 +0.000E+00-0.000E+00 1.218E+02 1.629E+02 +0.000E+00-0.000E+00 1.252E+02 1.788E+02 +0.000E+00-0.000E+00 1.298E+02 1.991E+02 +0.000E+00-0.000E+00 1.318E+02 2.204E+02 +0.000E+00-0.000E+00 1.373E+02 2.424E+02 +0.000E+00-0.000E+00 1.415E+02 2.659E+02 +0.000E+00-0.000E+00 \END; /*===================================================================*/ |