/*===================================================================*/ /* NRDF D1438 Data No.41 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,41; D#=D1438; TITLE=/COMPARISON OF GAMMA-RAY YIELD FUNCTIONS FOR THE 12C+24MG AND 16O+28SI REACTIONS/; PURPOSE=/TO EXPLORE THE EXTENT TO WHICH THESE STRUCTURES ARE PRESENT IN THE GAMMA-RAY YIELDS AND FOR HOW HEAVY A SYSTEM ARE THEY STILL OBSERVABLE BY THIS TECHNIQUE./; ATH=(R.M.FREEMAN'1',F.HAAS'1',B.HEUSCH'1',S.M.LEE'1'); INST-ATH=(2FR STR'1'); REF=PR/C; VLP=20(1979)569; RCTS=(12C(24MG,X)X,16O(28SI,X)X); PHQS=(EXC-FUNCT,INTNSTY-GAMMA,EXC-ENGY); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,41; RCT=12C(24MG,X)X; RTY=(SQNTL-RCT); ENR=NAT; CHM=ELM; PHYS-FORM=SLD; THK-TGT=55E-3MG/CM**2; BAC=AU; THK-BAC=XMG/CM**2; ACC=(VDGT); INST-ACC=2FR STR; INC-ENGY-LAB-RANGE=(45MEV(XMEV)71MEV); BEAM-INTNSTY=20E-9A; CHRG-INC-ION=5+; DET-PARTCL=(GAMMA); DET-SYS=(GE(LI)); EFCN-DET=/@32@/; PHQ=(EXC-FUNCT,YLD); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,41; CMPD=28SI; EMT-1=ALPHA; EMT-2=ALPHA; RSD=20NE; EXC-ENGY=1.79MEV; THTL=55DEG'41'; /*@51@*/ TOT-ERR=1%; /*FIG.3(B)*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; INC-ENGY-CM YLD DELTA-YLD (MEV) (MB) (MB) 1.498E+02 1.800E+02 +2.860E+00-2.430E+00 1.534E+02 1.859E+02 +3.004E+00-3.003E+00 1.564E+02 1.942E+02 +3.289E+00-2.717E+00 1.590E+02 2.001E+02 +2.716E+00-2.575E+00 1.622E+02 2.047E+02 +3.432E+00-2.287E+00 1.658E+02 2.127E+02 +2.576E+00-2.290E+00 1.695E+02 2.192E+02 +2.860E+00-3.290E+00 1.731E+02 2.330E+02 +2.002E+00-3.146E+00 1.760E+02 2.402E+02 +3.718E+00-3.004E+00 1.789E+02 2.455E+02 +2.860E+00-3.288E+00 1.821E+02 2.503E+02 +2.859E+00-2.861E+00 1.858E+02 2.562E+02 +3.290E+00-2.431E+00 1.897E+02 2.600E+02 +4.005E+00-3.146E+00 1.931E+02 2.723E+02 +3.862E+00-3.719E+00 1.958E+02 2.822E+02 +3.004E+00-3.289E+00 1.986E+02 2.844E+02 +2.289E+00-2.718E+00 2.023E+02 2.874E+02 +2.574E+00-2.287E+00 2.064E+02 2.884E+02 +2.862E+00-1.429E+00 2.101E+02 2.864E+02 +2.431E+00-3.719E+00 2.131E+02 2.971E+02 +3.004E+00-4.719E+00 2.158E+02 3.051E+02 +3.003E+00-3.288E+00 2.187E+02 3.158E+02 +4.290E+00-3.288E+00 2.227E+02 3.179E+02 +3.861E+00-3.001E+00 2.262E+02 3.236E+02 +3.860E+00-2.003E+00 2.300E+02 3.266E+02 +2.860E+00-2.002E+00 2.326E+02 3.216E+02 +3.431E+00-3.146E+00 2.352E+02 3.223E+02 +3.859E+00-2.717E+00 \END; /*===================================================================*/ |