/*===================================================================*/ /* NRDF D0357 Data No.1 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,1; D#=D357; TITLE=/APPLICATION OF THE CRYSTAL BLOCKING TECHNIQUE TO THE STUDY OF THE HIGHLY EXCITED NUCLEAR CONTINUUM/; PURPOSE=/TO EXAMINE CHANGES OF THE REACTION TIMES DUE TO ENHANCEMENT OF CERTAIN STATES AMONG THE MANY COMPOUND NUCLEAR FINE-STRUCTURE RESONANCES BY AN ISOBARIC ANALOGUE RESONANCE./; ATH=(W.M.GIBSON'1,2',M.MARUYAMA'3',Y.HASHIMOTO'3',E.P.KANTER'3', G.M.TEMMER'3',R.J.KEDDY'4',D.W.MINGAY'4',J.P.F.SELLSCHOP'4'); INST-ATH=(1USABEL'1',1USAALB'2',1USARUT'3',3SAFWIT'4'); /*@7@*/ REF=NP/A; VLP=317(1979)313; RCTS=(70GE(P,P)70GE,72GE(P,P)72GE,74GE(P,P)74GE); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,1; ENR=NAT; CHM=ELN; THK-TGT=X'1'; /*@8@*/ BAC=C'2'; /*@11@*/ POL-TGT=NO; ACC=(VDG); INST-ACC=1USARUT; INC-ENGY-LAB-RANGE=(5.035MEV,5.110MEV,4.200MEV,3.708MEV,4.358MEV, 5.210MEV); POL-PRJ=NO; DET-PARTCL=(P); DET-SYS=(PS-SI); ERS-DET=58KEV; ANL=(DWBA,STATIST-MODEL,X'1'); /*@9@*/ RCT=72GE(P,P)72GE; PHQ=(EXC-FUNCT,EXC-ENGY,SPIN,PTY); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,1; INC-ENGY-LAB=4.9[5.2MEV; CMPD=73AS; RSD=72GE; EXC-ENGY=0MEV; THTL=90DEG; /*FIG.1-(A)*/ /* D357 FIG.1-(A) */ /* SER#= 1 */ /* XSCALE=LINEAR YSCALE=LINEAR */ /* XMAX= 5.19999981E+00 YMAX= 2.00000000E+02 */ /* XMIN= 4.89999962E+00 YMIN= 1.50000000E+02 */ /* FOLLOWING DATA ARE TAKEN FROM GRAPH */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; INC-ENGY-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE (MEV) (MB/SR/MEV) (MB/SR/MEV) 4.901 2.076E+02 4.822E+00 4.904 2.109E+02 XXXXXXXXX 4.906 2.066E+02 XXXXXXXXX 4.909 2.036E+02 XXXXXXXXX 4.912 2.048E+02 XXXXXXXXX 4.915 2.036E+02 XXXXXXXXX 4.919 2.041E+02 XXXXXXXXX 4.923 2.018E+02 XXXXXXXXX 4.926 1.980E+02 XXXXXXXXX 4.928 2.000E+02 XXXXXXXXX 4.931 2.018E+02 XXXXXXXXX 4.935 1.995E+02 XXXXXXXXX 4.937 2.018E+02 XXXXXXXXX 4.938 1.985E+02 XXXXXXXXX 4.943 1.985E+02 XXXXXXXXX 4.945 2.013E+02 XXXXXXXXX 4.950 1.995E+02 XXXXXXXXX 4.951 1.934E+02 5.837E+00 4.954 1.919E+02 XXXXXXXXX 4.957 1.914E+02 XXXXXXXXX 4.960 1.962E+02 XXXXXXXXX 4.964 1.934E+02 XXXXXXXXX 4.967 1.886E+02 XXXXXXXXX 4.970 1.871E+02 XXXXXXXXX 4.973 1.881E+02 XXXXXXXXX 4.976 1.863E+02 XXXXXXXXX 4.977 1.843E+02 XXXXXXXXX 4.981 1.843E+02 XXXXXXXXX 4.983 1.794E+02 XXXXXXXXX 4.986 1.772E+02 XXXXXXXXX 4.990 1.728E+02 XXXXXXXXX 4.992 1.706E+02 XXXXXXXXX 4.995 1.650E+02 XXXXXXXXX 4.998 1.594E+02 XXXXXXXXX 5.001 1.581E+02 3.299E+00 5.004 1.607E+02 XXXXXXXXX 5.006 1.670E+02 XXXXXXXXX 5.011 1.708E+02 XXXXXXXXX 5.014 1.734E+02 XXXXXXXXX 5.017 1.751E+02 XXXXXXXXX 5.019 1.787E+02 XXXXXXXXX 5.022 1.812E+02 XXXXXXXXX 5.026 1.901E+02 XXXXXXXXX 5.028 1.977E+02 XXXXXXXXX 5.032 1.972E+02 XXXXXXXXX 5.035 2.003E+02 XXXXXXXXX 5.038 2.036E+02 XXXXXXXXX 5.040 2.036E+02 4.822E+00 5.044 2.028E+02 XXXXXXXXX 5.046 1.980E+02 XXXXXXXXX 5.050 1.972E+02 XXXXXXXXX 5.054 1.954E+02 XXXXXXXXX 5.056 1.898E+02 XXXXXXXXX 5.062 1.904E+02 XXXXXXXXX 5.065 1.850E+02 XXXXXXXXX 5.067 1.838E+02 XXXXXXXXX 5.070 1.802E+02 XXXXXXXXX 5.073 1.716E+02 XXXXXXXXX 5.075 1.645E+02 XXXXXXXXX 5.079 1.617E+02 XXXXXXXXX 5.083 1.561E+02 XXXXXXXXX 5.086 1.561E+02 XXXXXXXXX 5.089 1.482E+02 XXXXXXXXX 5.091 1.467E+02 XXXXXXXXX 5.094 1.454E+02 XXXXXXXXX 5.097 1.437E+02 XXXXXXXXX 5.100 1.437E+02 3.553E+00 5.103 1.434E+02 XXXXXXXXX 5.106 1.482E+02 XXXXXXXXX 5.108 1.510E+02 XXXXXXXXX 5.111 1.561E+02 XXXXXXXXX 5.116 1.589E+02 XXXXXXXXX 5.118 1.642E+02 XXXXXXXXX 5.121 1.703E+02 XXXXXXXXX 5.124 1.718E+02 XXXXXXXXX 5.127 1.741E+02 XXXXXXXXX 5.130 1.754E+02 XXXXXXXXX 5.134 1.751E+02 XXXXXXXXX 5.138 1.756E+02 XXXXXXXXX 5.140 1.766E+02 XXXXXXXXX 5.143 1.777E+02 XXXXXXXXX 5.146 1.797E+02 XXXXXXXXX 5.149 1.794E+02 XXXXXXXXX 5.153 1.799E+02 4.060E+00 5.155 1.817E+02 XXXXXXXXX 5.159 1.792E+02 XXXXXXXXX 5.162 1.815E+02 XXXXXXXXX 5.164 1.777E+02 XXXXXXXXX 5.167 1.772E+02 XXXXXXXXX 5.170 1.772E+02 XXXXXXXXX 5.173 1.789E+02 XXXXXXXXX 5.177 1.820E+02 XXXXXXXXX 5.181 1.830E+02 XXXXXXXXX 5.182 1.766E+02 XXXXXXXXX 5.187 1.766E+02 XXXXXXXXX 5.189 1.772E+02 XXXXXXXXX 5.191 1.751E+02 XXXXXXXXX 5.195 1.756E+02 XXXXXXXXX 5.198 1.764E+02 4.568E+00 \END; /*===================================================================*/ |