/*===================================================================*/ /* NRDF D1672 Data No.14 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,14; 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,14; 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,14; INC-ENGY-LAB=6MEV; EMT-1=D; RSD=X; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DATA3'43' DELTA-DATA3 (DEG) (NODIM) (NODIM) 2.032E+01 1.223E-02 +5.377E-04-3.222E-04 2.310E+01 1.317E-02 +4.303E-04-4.659E-04 2.685E+01 1.432E-02 +6.450E-04-4.838E-04 3.059E+01 1.444E-02 +3.401E-04-2.329E-04 3.385E+01 1.455E-02 +4.840E-04-4.300E-04 3.734E+01 1.451E-02 +4.299E-04-3.763E-04 3.992E+01 1.264E-02 +4.123E-04-5.197E-04 4.276E+01 1.260E-02 +2.866E-04-3.045E-04 4.542E+01 1.097E-02 +2.151E-04-2.329E-04 4.825E+01 9.859E-03 +2.150E-04-1.076E-04 5.165E+01 8.297E-03 +2.147E-04-3.225E-04 5.464E+01 7.489E-03 +1.612E-04-2.870E-04 5.876E+01 5.801E-03 +0.000E+00-0.000E+00 6.314E+01 4.813E-03 +2.150E-04-2.331E-04 6.720E+01 4.182E-03 +1.254E-04-2.511E-04 7.060E+01 3.481E-03 +1.792E-04-2.689E-04 7.450E+01 3.120E-03 +2.689E-04-1.971E-04 7.791E+01 2.992E-03 +3.047E-04-2.867E-04 8.142E+01 3.725E-03 +1.971E-04-3.047E-04 8.730E+01 6.104E-03 +1.613E-04-3.767E-04 9.007E+01 5.941E-03 +3.944E-04-7.889E-04 9.262E+01 7.946E-03 +1.613E-04-2.689E-04 9.498E+01 8.715E-03 +4.838E-04-6.093E-04 9.846E+01 1.269E-02 +5.018E-04-6.453E-04 1.028E+02 1.557E-02 +6.807E-04-6.453E-04 1.064E+02 1.681E-02 +4.122E-04-5.016E-04 1.106E+02 1.964E-02 +4.299E-04-6.090E-04 1.139E+02 1.974E-02 +4.841E-04-4.662E-04 1.172E+02 2.094E-02 +4.299E-04-5.379E-04 1.216E+02 1.823E-02 +4.297E-04-6.100E-04 1.252E+02 1.665E-02 +5.018E-04-4.296E-04 1.274E+02 1.407E-02 +3.944E-04-2.866E-04 1.290E+02 1.358E-02 +5.016E-04-8.241E-04 1.314E+02 1.235E-02 +5.020E-04-5.196E-04 1.336E+02 8.473E-03 +6.987E-04-6.812E-04 1.354E+02 6.554E-03 +5.375E-04-8.422E-04 1.371E+02 5.173E-03 +6.094E-04-5.021E-04 1.386E+02 3.452E-03 +6.809E-04-5.377E-04 1.402E+02 1.049E-03 +6.807E-04-6.094E-04 1.421E+02 1.729E-03 +4.122E-04-3.942E-04 1.440E+02 -4.409E-04 +5.734E-04-4.839E-04 1.463E+02 -1.159E-03 +5.555E-04-6.271E-04 1.478E+02 -3.365E-03 +1.434E-04-3.229E-04 1.499E+02 -3.492E-03 +1.972E-04-1.074E-04 1.516E+02 -3.690E-03 +1.614E-04-2.510E-04 1.520E+02 -4.192E-03 +1.254E-04-2.329E-04 1.532E+02 -4.462E-03 +1.792E-04-1.433E-04 1.540E+02 -4.892E-03 +1.613E-04-2.151E-04 1.561E+02 -5.593E-03 +2.865E-04-2.870E-04 1.589E+02 -6.276E-03 +3.046E-04-5.198E-04 1.615E+02 -5.310E-03 +1.971E-04-2.866E-04 1.633E+02 -5.203E-03 +5.199E-04-5.736E-04 1.647E+02 -5.402E-03 +0.000E+00-0.000E+00 1.672E+02 -5.224E-03 +6.990E-04-3.944E-04 \END; /*===================================================================*/ |