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 /* NRDF D1547 Data No.26                                             */
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 /* Bibliography                                                      */
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 \\BIB,26;
 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@*/
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 /* Experimental Conditions                                           */
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 \\EXP,26;
 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,26;
 INC-ENGY-LAB=25MEV;
 RSD=21NA;
 EXC-ENGY-INITL=6.51MEV;
 J-PTY-INITL=3/2+;
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 /* Data Table                                                        */
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 \DATA;
 THTC'11'  DSIGMA/DOMEGA  DELTA-DSIGMA/DOMEGA
 (DEG)   (B/SR)       (B/SR)
  1.928E+00  1.026E+01  +0.000E+00-0.000E+00
  8.502E+00  7.192E+00  +0.000E+00-0.000E+00
  1.100E+01  6.419E+00  +0.000E+00-0.000E+00
  1.415E+01  3.686E+00  +0.000E+00-0.000E+00
  1.720E+01  2.962E+00  +0.000E+00-0.000E+00
  2.100E+01  2.215E+00  +0.000E+00-0.000E+00
  2.553E+01  1.299E+00  +0.000E+00-0.000E+00
  2.860E+01  1.239E+00  +0.000E+00-0.000E+00
  3.192E+01  5.718E-01  +6.071E-02-3.238E-02
  3.717E+01  5.437E-01  +6.433E-02-5.780E-02
  4.198E+01  3.687E-01  +4.328E-02-3.734E-02
  4.663E+01  3.061E-01  +3.593E-02-3.391E-02
  5.150E+01  1.740E-01  +1.660E-02-1.924E-02
  5.804E+01  1.551E-01  +2.274E-02-1.497E-02
  6.378E+01  8.615E-02  +9.710E-03-7.546E-03
  6.866E+01  8.051E-02  +0.000E+00-0.000E+00
  7.330E+01  9.257E-02  +0.000E+00-0.000E+00
  7.803E+01  7.687E-02  +0.000E+00-0.000E+00
 \END;
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