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| /*===================================================================*/
/* 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;
/*===================================================================*/
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