/*===================================================================*/ /* NRDF D1672 Data No.12 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,12; 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,12; 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'42'; /*@42@*/ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,12; INC-ENGY-LAB=6MEV; EMT-1=D; RSD=X; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DATA2'42' DELTA-DATA2 (DEG) (NODIM) (NODIM) 2.211E+01 -4.501E-02 +0.000E+00-0.000E+00 2.577E+01 -4.360E-02 +0.000E+00-0.000E+00 2.775E+01 -3.877E-02 +0.000E+00-0.000E+00 2.965E+01 -3.433E-02 +0.000E+00-0.000E+00 3.276E+01 -2.993E-02 +0.000E+00-0.000E+00 3.610E+01 -2.499E-02 +1.785E-04-2.499E-04 3.928E+01 -2.040E-02 +0.000E+00-0.000E+00 4.234E+01 -1.728E-02 +0.000E+00-0.000E+00 4.619E+01 -1.387E-02 +0.000E+00-0.000E+00 4.960E+01 -1.179E-02 +0.000E+00-0.000E+00 5.292E+01 -9.917E-03 +0.000E+00-0.000E+00 5.628E+01 -9.402E-03 +0.000E+00-0.000E+00 5.942E+01 -9.601E-03 +3.209E-04-5.704E-04 6.213E+01 -8.768E-03 +0.000E+00-0.000E+00 6.549E+01 -8.431E-03 +0.000E+00-0.000E+00 6.911E+01 -8.915E-03 +1.778E-04-4.295E-04 7.315E+01 -1.025E-02 +2.506E-04-4.298E-04 7.793E+01 -1.191E-02 +0.000E+00-0.000E+00 8.303E+01 -1.406E-02 +0.000E+00-0.000E+00 8.757E+01 -1.590E-02 +0.000E+00-0.000E+00 8.931E+01 -1.486E-02 +3.584E-04-4.648E-04 9.158E+01 -1.581E-02 +0.000E+00-0.000E+00 9.324E+01 -1.480E-02 +3.930E-04-3.573E-04 9.608E+01 -1.615E-02 +6.072E-04-5.708E-04 1.003E+02 -1.495E-02 +6.068E-04-5.009E-04 1.042E+02 -8.969E-03 +6.782E-04-8.214E-04 1.087E+02 -4.878E-03 +0.000E+00-0.000E+00 1.131E+02 1.175E-03 +1.781E-04-3.562E-04 1.172E+02 6.120E-03 +3.930E-04-3.930E-04 1.210E+02 1.124E-02 +3.908E-04-4.998E-04 1.237E+02 1.447E-02 +0.000E+00-0.000E+00 1.257E+02 1.569E-02 +5.708E-04-6.797E-04 1.272E+02 1.809E-02 +5.355E-04-5.701E-04 1.293E+02 1.960E-02 +3.216E-04-4.287E-04 1.312E+02 1.829E-02 +2.142E-04-4.295E-04 1.330E+02 1.947E-02 +2.491E-04-4.276E-04 1.350E+02 1.791E-02 +0.000E+00-0.000E+00 1.371E+02 1.849E-02 +4.663E-04-1.789E-04 1.399E+02 1.758E-02 +4.317E-04-4.284E-04 1.423E+02 1.655E-02 +4.641E-04-7.496E-04 1.441E+02 1.649E-02 +3.577E-04-3.213E-04 1.466E+02 1.475E-02 +6.433E-04-6.072E-04 1.487E+02 1.458E-02 +3.938E-04-3.216E-04 1.504E+02 1.316E-02 +4.287E-04-4.633E-04 1.531E+02 1.128E-02 +3.573E-04-5.365E-04 1.543E+02 9.788E-03 +3.216E-04-2.491E-04 1.565E+02 8.299E-03 +5.693E-04-5.347E-04 1.580E+02 8.091E-03 +3.562E-04-5.001E-04 1.596E+02 8.171E-03 +4.641E-04-5.362E-04 1.612E+02 4.572E-03 +4.994E-04-7.121E-04 1.633E+02 5.438E-03 +5.355E-04-4.287E-04 \END; /*===================================================================*/ |