/*===================================================================*/ /* NRDF D1672 Data No.2 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,2; 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,2; 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,2; INC-ENGY-LAB=2MEV; EMT-1=P; RSD=X; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 2.567E+01 3.939E+02 +3.469E+00-2.439E+00 2.913E+01 3.181E+02 +0.000E+00-0.000E+00 3.229E+01 2.793E+02 +0.000E+00-0.000E+00 3.491E+01 2.520E+02 +0.000E+00-0.000E+00 3.689E+01 2.324E+02 +0.000E+00-0.000E+00 4.012E+01 2.205E+02 +0.000E+00-0.000E+00 4.262E+01 2.091E+02 +0.000E+00-0.000E+00 4.512E+01 1.995E+02 +0.000E+00-0.000E+00 4.764E+01 1.933E+02 +0.000E+00-0.000E+00 5.096E+01 1.847E+02 +0.000E+00-0.000E+00 5.452E+01 1.771E+02 +0.000E+00-0.000E+00 5.711E+01 1.687E+02 +0.000E+00-0.000E+00 6.027E+01 1.617E+02 +0.000E+00-0.000E+00 6.303E+01 1.568E+02 +0.000E+00-0.000E+00 6.628E+01 1.509E+02 +0.000E+00-0.000E+00 6.921E+01 1.482E+02 +0.000E+00-0.000E+00 7.123E+01 1.430E+02 +0.000E+00-0.000E+00 7.318E+01 1.385E+02 +0.000E+00-0.000E+00 7.765E+01 1.327E+02 +0.000E+00-0.000E+00 8.187E+01 1.270E+02 +0.000E+00-0.000E+00 8.619E+01 1.234E+02 +0.000E+00-0.000E+00 9.075E+01 1.229E+02 +0.000E+00-0.000E+00 9.605E+01 1.224E+02 +0.000E+00-0.000E+00 9.948E+01 1.242E+02 +0.000E+00-0.000E+00 1.025E+02 1.297E+02 +0.000E+00-0.000E+00 1.061E+02 1.341E+02 +0.000E+00-0.000E+00 1.100E+02 1.420E+02 +0.000E+00-0.000E+00 1.145E+02 1.506E+02 +0.000E+00-0.000E+00 1.188E+02 1.634E+02 +0.000E+00-0.000E+00 1.236E+02 1.794E+02 +0.000E+00-0.000E+00 1.280E+02 1.954E+02 +0.000E+00-0.000E+00 1.322E+02 2.147E+02 +0.000E+00-0.000E+00 1.359E+02 2.344E+02 +0.000E+00-0.000E+00 1.388E+02 2.561E+02 +0.000E+00-0.000E+00 1.421E+02 2.799E+02 +0.000E+00-0.000E+00 1.460E+02 3.008E+02 +0.000E+00-0.000E+00 \END; /*===================================================================*/ |