DARPE: Search Results
 /*===================================================================*/
 /* NRDF D1444 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1444;
 TITLE=/INCOMPLETE FUSION OF THE 16O+27AL REACTION/;
 PURPOSE=/TO OBTAIN INFORMATION ON THE ROLE OF THE ENTRANCE-CHANNEL
          ANGULAR MOMENTUM IN THE INCOMPLETE REACTION BY MEASURING THE
          VELOCITY DEFICTS OF THE PARTICLE EVAPOLATION PROCESSES./;
 ATH=(H.IKEZOE'1',N.SHIKAZONO'1',Y.TOMITA'1',K.IDENO'1',Y.SUGIYAMA'1',
      E.TAKEKOSHI'1');
 INST-ATH=(2JPNJAE'1');
 REF=NP/A;
 VLP=444(1985)349;
 RCTS=(27AL(16O,X)X);
 PHQS=(MOM-DSTRN,A-DSTRN,Z-DSTRN,DATA'1',FISSN-XSECTN);
 /*@1@*/
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 RCT=27AL(16O,X)X;
 RTY=(FUSN);
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=180MG/CM**2;
 BAC=SELF;
 POL-TGT=0%;
 ACC=(TVDG);
 INST-ACC=2JPNJAE;
 INC-ENGY-LAB=(90MEV'22',150MEV);
 /*@22@*/
 DET-PARTCL=(X'12');
 /*@12@*/
 DET-SYS=(TOF+EDE,SBD,IC)'13';
 /*@13@*/
 CALB-DET=/@15@/;
 MONTR-RCT=/@16@/;
 EFCN-DET=/@14@/;
 ANL=(OPT-MODEL,STATIST-MODEL);
 PHQ=(MOM-DSTRN,A-DSTRN,Z-DSTRN,DATA'1');
 /*@1@*/
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 INC-ENGY-LAB=150MEV;
 THTL=8DEG'2';
 /*@2@*/
 /*FIG.4A-2*/
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 /* Data Table                                                        */
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 \DATA;
 MASS  DATA'1' DELTA-DATA'1'
 (NODIM)  (NODIM)  (NODIM)
  2.786E+01 -8.068E+00  +-1.930E+00
  2.884E+01 -7.388E+00  +-1.910E+00
  2.992E+01 -7.838E+00  +-1.925E+00
  3.085E+01 -4.433E+00  +-1.689E+00
  3.193E+01 -5.162E+00  +-1.825E+00
  3.286E+01 -4.337E+00  +-1.925E+00
  3.393E+01 -4.302E+00  +-1.803E+00
  3.494E+01 -4.585E+00  +-1.506E+00
  3.602E+01 -3.247E+00  +-1.532E+00
  3.695E+01 -2.087E+00  +-1.334E+00
  3.805E+01  4.909E-01  +-1.296E+00
 \END;
 /*===================================================================*/