/*===================================================================*/ /* NRDF D1672 Data No.3 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,3; 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,3; 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,3; INC-ENGY-LAB=3MEV; EMT-1=P; RSD=X; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 2.275E+01 3.116E+02 +0.000E+00-0.000E+00 2.509E+01 2.684E+02 +0.000E+00-0.000E+00 2.921E+01 2.445E+02 +0.000E+00-0.000E+00 3.215E+01 2.288E+02 +0.000E+00-0.000E+00 3.486E+01 2.180E+02 +0.000E+00-0.000E+00 3.760E+01 2.110E+02 +0.000E+00-0.000E+00 3.983E+01 2.024E+02 +0.000E+00-0.000E+00 4.249E+01 1.958E+02 +0.000E+00-0.000E+00 4.505E+01 1.878E+02 +0.000E+00-0.000E+00 4.819E+01 1.792E+02 +0.000E+00-0.000E+00 5.093E+01 1.740E+02 +0.000E+00-0.000E+00 5.447E+01 1.668E+02 +0.000E+00-0.000E+00 5.745E+01 1.596E+02 +0.000E+00-0.000E+00 6.026E+01 1.522E+02 +0.000E+00-0.000E+00 6.324E+01 1.458E+02 +0.000E+00-0.000E+00 6.638E+01 1.401E+02 +0.000E+00-0.000E+00 6.896E+01 1.351E+02 +0.000E+00-0.000E+00 7.113E+01 1.302E+02 +0.000E+00-0.000E+00 7.329E+01 1.224E+02 +0.000E+00-0.000E+00 7.804E+01 1.115E+02 +0.000E+00-0.000E+00 8.150E+01 1.033E+02 +0.000E+00-0.000E+00 8.578E+01 9.645E+01 +0.000E+00-0.000E+00 9.038E+01 9.043E+01 +0.000E+00-0.000E+00 9.452E+01 8.869E+01 +0.000E+00-0.000E+00 9.930E+01 8.592E+01 +0.000E+00-0.000E+00 1.029E+02 8.623E+01 +0.000E+00-0.000E+00 1.065E+02 8.674E+01 +0.000E+00-0.000E+00 1.100E+02 8.807E+01 +0.000E+00-0.000E+00 1.138E+02 9.488E+01 +0.000E+00-0.000E+00 1.178E+02 1.025E+02 +0.000E+00-0.000E+00 1.231E+02 1.133E+02 +0.000E+00-0.000E+00 1.277E+02 1.295E+02 +0.000E+00-0.000E+00 1.313E+02 1.454E+02 +0.000E+00-0.000E+00 1.356E+02 1.628E+02 +0.000E+00-0.000E+00 1.389E+02 1.853E+02 +0.000E+00-0.000E+00 1.424E+02 2.102E+02 +0.000E+00-0.000E+00 1.463E+02 2.314E+02 +0.000E+00-0.000E+00 \END; /*===================================================================*/ |