/*===================================================================*/ /* NRDF D1672 Data No.13 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,13; 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,13; 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'43'; /*@43@*/ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,13; INC-ENGY-LAB=5MEV; EMT-1=D; RSD=X; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DATA3'43' DELTA-DATA3 (DEG) (NODIM) (NODIM) 1.885E+01 1.114E-02 +9.161E-04-8.808E-04 2.104E+01 1.233E-02 +3.235E-04-3.594E-04 2.478E+01 1.233E-02 +4.851E-04-6.108E-04 2.891E+01 1.362E-02 +7.008E-04-5.930E-04 3.209E+01 1.318E-02 +7.905E-04-4.675E-04 3.510E+01 1.260E-02 +5.391E-04-5.032E-04 3.812E+01 1.163E-02 +4.492E-04-3.414E-04 4.137E+01 1.192E-02 +4.311E-04-3.416E-04 4.365E+01 1.072E-02 +5.931E-04-5.571E-04 4.675E+01 9.444E-03 +3.775E-04-3.773E-04 5.026E+01 8.403E-03 +2.875E-04-5.389E-04 5.409E+01 7.452E-03 +5.210E-04-5.390E-04 5.824E+01 6.735E-03 +5.031E-04-3.234E-04 6.214E+01 6.449E-03 +4.313E-04-5.031E-04 6.597E+01 5.498E-03 +5.391E-04-2.874E-04 6.963E+01 4.889E-03 +4.851E-04-7.009E-04 7.313E+01 4.782E-03 +3.953E-04-3.234E-04 7.711E+01 5.000E-03 +3.414E-04-4.672E-04 8.100E+01 6.870E-03 +4.131E-04-4.313E-04 8.555E+01 7.699E-03 +4.673E-04-4.674E-04 9.122E+01 1.040E-02 +4.493E-04-3.415E-04 9.404E+01 1.347E-02 +4.672E-04-3.775E-04 9.711E+01 1.493E-02 +4.313E-04-2.875E-04 1.008E+02 1.647E-02 +5.031E-04-5.391E-04 1.039E+02 1.885E-02 +4.490E-04-5.392E-04 1.081E+02 1.863E-02 +3.953E-04-4.491E-04 1.119E+02 1.925E-02 +6.287E-04-9.525E-04 1.153E+02 1.700E-02 +5.211E-04-6.290E-04 1.204E+02 1.459E-02 +5.567E-04-5.750E-04 1.250E+02 1.134E-02 +5.751E-04-7.368E-04 1.277E+02 1.149E-02 +0.000E+00-0.000E+00 1.296E+02 1.023E-02 +7.904E-04-6.830E-04 1.322E+02 8.616E-03 +7.725E-04-8.987E-04 1.339E+02 6.244E-03 +7.548E-04-3.235E-04 1.359E+02 3.604E-03 +6.828E-04-8.091E-04 1.379E+02 3.586E-03 +7.549E-04-7.189E-04 1.390E+02 1.215E-03 +8.090E-04-7.369E-04 1.410E+02 2.812E-04 +5.392E-04-5.929E-04 1.428E+02 7.671E-04 +7.366E-04-3.953E-04 1.449E+02 -4.720E-04 +5.212E-04-5.931E-04 1.470E+02 -1.837E-03 +5.211E-04-5.032E-04 1.495E+02 -2.968E-03 +5.931E-04-7.733E-04 1.508E+02 -3.560E-03 +6.290E-04-3.773E-04 1.535E+02 -2.733E-03 +8.265E-04-3.597E-04 1.575E+02 -3.216E-03 +4.135E-04-5.570E-04 1.622E+02 -2.406E-03 +6.108E-04-6.113E-04 1.646E+02 -2.441E-03 +5.391E-04-6.652E-04 1.664E+02 -3.231E-03 +1.078E-03-1.186E-03 \END; /*===================================================================*/ |