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 /* NRDF D0120 Data No.20                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,20;
 D#=D1547;
 TITLE=/PROTON SINGLE-PARTICLE STATES IN 21,23NA THROUGH THE
       (D,N) REACTION/;
 PURPOSE=/TO SEE THE SINGLE-PARTICLE OR SINGLE-HOLE STATES IN RESIDUAL
          NUCLEI AND GROUND-STATE PROPERTIES OF THE TARGET NUCLEUS./;
 ATH=(A.TERAKAWA'1',T.TOHEI'1',T.NAKAGAWA'1',A.SATO'1',J.TAKAMATSU'1',
      M.MORI'1',A.NARITA'1',H.ORIHARA'2',K.ISHII'2',T.NIIZEKI'2',
      M.OURA'2',S.HIRASAKI'2',M.HOSAKA'2',G.C.JON'2',K.MIURA'3',
      H.OHNUMA'4');
 INST-ATH=(2JPNTOH'1',2JPNTOH'2',2JPNTOI'3',2JPNTIT'4');
 /*@1@*/
 /*@2@*/
 REF=PR/C;
 VLP=48(1993)2775;
 RCTS=(20NE(D,N)21NA,22NE(D,N)23NA);
 PHQS=(ANGL-DSTRN,SPEC-STR'21');
 /*@22@*/
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,20;
 RCT=20NE(D,N)21NA;
 RTY=(INEL-SCATT);
 ENR=99.9%;
 CHM=ELM;
 PHYS-FORM=GAS;
 THK-TGT=1.0MG/CM**2;
 BAC=SELF;
 ACC=(CYC);
 INST-ACC=2JPNTOH;
 INC-ENGY-LAB=(25MEV);
 CHRG-INC-ION=1;
 DET-PARTCL=(N);
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(TOF)'1';
 /*@12@*/
 SOLID-ANGL=0.23MSR;
 /* EFCN-DET=DETECTOR EFFICIENCY WAS 3% WHICH WAS DETERMINED BY THE
 7LI(P,N)7BE REACTION THROUGH ACTIVATION ANALYSIS. */
 ANL=(OPT-MODEL,ADBA'2',DWBA);
 /*@13@*/
 PHQ=(ANGL-DSTRN,SPEC-STR'21');
 /*@22@*/
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,20;
 INC-ENGY-LAB=25MEV;
 RSD=21NA;
 EXC-ENGY-INITL=4.17MEV;
 J-PTY-INITL=3/2-;
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 /* Data Table                                                        */
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 \DATA;
 THTC'7'  DSIGMA/DOMEGA  DELTA-DSIGMA/DOMEGA
 (DEG)   (B/SR)       (B/SR)
  2.236E+00  9.621E+00  +0.000E+00-0.000E+00
  4.436E+00  1.084E+01  +0.000E+00-0.000E+00
  1.292E+01  5.211E+00  +0.000E+00-0.000E+00
  1.495E+01  3.286E+00  +0.000E+00-0.000E+00
  1.778E+01  2.302E+00  +0.000E+00-0.000E+00
  2.033E+01  1.551E+00  +0.000E+00-0.000E+00
  2.334E+01  1.218E+00  +0.000E+00-0.000E+00
  2.595E+01  9.605E-01  +0.000E+00-0.000E+00
  2.918E+01  6.697E-01  +0.000E+00-0.000E+00
  3.312E+01  6.134E-01  +0.000E+00-0.000E+00
  3.903E+01  4.747E-01  +0.000E+00-0.000E+00
  4.484E+01  2.756E-01  +2.662E-02-2.021E-02
  4.991E+01  1.741E-01  +2.416E-02-2.283E-02
  5.371E+01  2.113E-01  +0.000E+00-0.000E+00
  5.876E+01  1.185E-01  +1.871E-02-1.105E-02
  6.434E+01  1.096E-01  +0.000E+00-0.000E+00
  7.004E+01  9.245E-02  +0.000E+00-0.000E+00
  7.607E+01  6.527E-02  +0.000E+00-0.000E+00
  8.068E+01  4.097E-02  +6.964E-03-3.019E-03
 \END;
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