/*===================================================================*/
 /* NRDF D1438 Data No.42                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,42;
 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,42;
 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,42;
 CMPD=31P;
 EMT-1=ALPHA;
 EMT-2=P;
 RSD=26MG;
 EXC-ENGY=1.27MEV;
 THTL=55DEG'41';
 /*@51@*/
 TOT-ERR=1%;
 /*FIG.3(C)*/
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-CM YLD DELTA-YLD
 (MEV) (MB)  (MB)
  1.495E+02  1.266E+02  +3.719E+00-1.860E+00
  1.532E+02  1.330E+02  +2.717E+00-1.716E+00
  1.562E+02  1.435E+02  +2.146E+00-2.145E+00
  1.589E+02  1.550E+02  +1.574E+00-2.288E+00
  1.622E+02  1.625E+02  +2.719E+00-3.004E+00
  1.658E+02  1.654E+02  +2.574E+00-2.288E+00
  1.696E+02  1.781E+02  +2.575E+00-2.574E+00
  1.731E+02  1.855E+02  +2.005E+00-2.860E+00
  1.759E+02  1.938E+02  +3.432E+00-3.432E+00
  1.786E+02  2.005E+02  +2.573E+00-1.575E+00
  1.822E+02  2.039E+02  +3.290E+00-2.431E+00
  1.861E+02  2.040E+02  +3.431E+00-3.574E+00
  1.898E+02  2.088E+02  +3.289E+00-2.289E+00
  1.930E+02  2.118E+02  +3.575E+00-3.003E+00
  1.957E+02  2.192E+02  +4.291E+00-3.718E+00
  1.987E+02  2.198E+02  +2.145E+00-3.861E+00
  2.021E+02  2.199E+02  +2.575E+00-3.718E+00
  2.063E+02  2.116E+02  +3.575E+00-2.717E+00
  2.100E+02  2.136E+02  +3.146E+00-4.718E+00
  2.130E+02  2.167E+02  +3.575E+00-2.145E+00
  2.155E+02  2.131E+02  +4.432E+00-3.289E+00
  2.187E+02  2.178E+02  +3.575E+00-4.147E+00
  2.227E+02  2.147E+02  +3.720E+00-2.002E+00
  2.266E+02  2.129E+02  +4.577E+00-2.002E+00
  2.299E+02  2.106E+02  +2.717E+00-3.716E+00
  2.326E+02  2.086E+02  +3.574E+00-3.718E+00
  2.354E+02  2.044E+02  +3.575E+00-4.863E+00
 \END;
 /*===================================================================*/