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 /* NRDF D1551 Data No.3                                              */
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 /* Bibliography                                                      */
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 \\BIB,3;
 D#=D1551;
 TITLE=/SYMMETRIC MASS-DIVISION PROCESS IN NUCLEI WITH MASS NUMBERS
        AROUND A(CN)=100/;
 PURPOSE=/TO ELUCIDATE THE PRESENCE OF THE SYMMETRIC MASS-DIVISION
          PROCESS IN LIGHT NUCLEI WITH MASS NUMBERS OF THE COMPOUND
          NUCLEUS A(CN)=100 AND TO STUDY THE ROLE OF ANGULAR MOMENTUM./;
 ATH=(Y.NAGAME'1',H.IKEZOE'1',T.OHTSUKI'1,2');
 INST-ATH=(2JPNJAE'1');
 /*@2@*/
 REF=PR/C;
 VLP=47(1993)1586;
 RCTS=(68ZN(37CL,X)X,89Y(16O,X)X);
 PHQS=(A-DSTRN,ANGL-DSTRN,TOT-KIN-ENGY)'15';
 /*@15@*/
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,3;
 RCT=68ZN(37CL,X)X;
 RTY=(CMPD-RCT,FISSN);
 ENR=99.34%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=755E-3MG/CM**2;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(VDGT);
 INST-ACC=2JPNJAE;
 INC-ENGY-LAB=(160MEV,177MEV);
 ERS-PRJ=XKEV;
 BEAM-INTNSTY=XA;
 CHRG-INC-ION=+17;
 POL-PRJ=0%;
 DET-PARTCL=(X'20');
 /*@20@*/
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SBD,TOF);
 SOLID-ANGL=XMSR;
 ERS-DET=XKEV;
 CALB-DET=/@THE ENERGY CALIBRATION WAS PERFORMED BY USING THE
           ELASTICALLY SCATTERD PROJECTILES FRON A
           100-MICROGRAM/CM**2-THICK 197AU TARGET AT HIGH ENERGIES AND
           ALPHA PARTICLES FROM AN 241AM SOURCE AT LOW ENERGY.@/;
 ANL=(STATIST-MODEL);
 PHQ=(DSIGMA/DOMEGA);
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,3;
 INC-ENGY-LAB=160MEV;
 CMPD=105AG;
 EMT=X'20';
 RSD=X'20';
 /*@20@*/
 THTL=20DEG;
 NORM=X'30';
 /*@30@*/
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 /* Data Table                                                        */
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 \DATA;
 MASS  DSIGMA/DOMEGA  DELTA-DSIGMA/DOMEGA
 (NODIM) (MB/SR)       (MB/SR)
  5.100E+01  1.662E+00  +1.350E-01-1.350E-01
  5.300E+01  1.601E+00  +9.931E-02-9.931E-02
  5.500E+01  1.590E+00  +1.117E-01-1.117E-01
  5.700E+01  1.472E+00  +8.705E-02-8.705E-02
  5.900E+01  1.404E+00  +9.710E-02-9.710E-02
  6.100E+01  1.226E+00  +1.128E-01-1.128E-01
  6.300E+01  1.243E+00  +8.916E-02-8.916E-02
  6.500E+01  1.159E+00  +7.703E-02-7.703E-02
  6.700E+01  1.103E+00  +9.719E-02-9.719E-02
  6.900E+01  9.183E-01  +7.590E-02-7.590E-02
  7.100E+01  9.056E-01  +9.368E-02-9.368E-02
  7.300E+01  6.552E-01  +7.576E-02-7.576E-02
  7.400E+01  5.177E-01  +5.695E-02-5.695E-02
  7.600E+01  3.699E-01  +3.563E-02-3.563E-02
 \END;
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