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 /* NRDF D1547 Data No.66                                             */
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 /* Bibliography                                                      */
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 \\BIB,66;
 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,66;
 RCT=22NE(D,N)23NA;
 RTY=(INEL-SCATT);
 ENR=99.9%;
 CHM=ELM;
 PHYS-FORM=GAS;
 THK-TGT=1.1MG/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                                            */
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 \\DATA,66;
 INC-ENGY-LAB=25MEV;
 RSD=23NA;
 EXC-ENGY-INITL=10.94MEV;
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 /* Data Table                                                        */
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 \DATA;
 THTC'15'  DSIGMA/DOMEGA  DELTA-DSIGMA/DOMEGA
 (DEG)   (B/SR)       (B/SR)
  1.226E+01  2.880E+00  +0.000E+00-0.000E+00
  1.392E+01  2.425E+00  +0.000E+00-0.000E+00
  1.649E+01  2.797E+00  +0.000E+00-0.000E+00
  1.970E+01  1.604E+00  +0.000E+00-0.000E+00
  2.361E+01  1.283E+00  +0.000E+00-0.000E+00
  2.698E+01  8.927E-01  +0.000E+00-0.000E+00
  3.025E+01  6.034E-01  +0.000E+00-0.000E+00
  3.346E+01  4.486E-01  +6.506E-02-7.366E-02
  4.283E+01  2.767E-01  +3.667E-02-4.202E-02
  4.915E+01  2.012E-01  +4.669E-02-3.056E-02
  5.434E+01  1.700E-01  +2.972E-02-2.635E-02
  5.852E+01  1.330E-01  +1.436E-02-2.506E-02
  6.323E+01  9.466E-02  +1.777E-02-1.811E-02
 \END;
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