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 /* NRDF D1547 Data No.18                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,18;
 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                                           */
 /*===================================================================*/
 \\EXP,18;
 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,18;
 INC-ENGY-LAB=25MEV;
 RSD=21NA;
 EXC-ENGY-INITL=2.80MEV;
 J-PTY-INITL=1/2-;
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 /* Data Table                                                        */
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 \DATA;
 THTC'7'  DSIGMA/DOMEGA  DELTA-DSIGMA/DOMEGA
 (DEG)   (B/SR)       (B/SR)
  1.640E+01  1.020E+00  +1.528E-01-2.341E-01
  1.900E+01  1.036E+00  +1.496E-01-8.961E-02
  2.246E+01  7.467E-01  +1.347E-01-6.114E-02
  2.499E+01  6.852E-01  +1.249E-01-7.567E-02
  2.917E+01  5.335E-01  +9.191E-02-6.905E-02
  3.227E+01  6.339E-01  +0.000E+00-0.000E+00
  3.666E+01  4.254E-01  +3.303E-02-2.229E-02
  4.272E+01  3.409E-01  +3.203E-02-5.967E-02
  4.813E+01  3.032E-01  +3.561E-02-3.907E-02
  5.237E+01  2.892E-01  +3.256E-02-2.492E-02
  5.742E+01  2.966E-01  +0.000E+00-0.000E+00
  6.330E+01  1.679E-01  +2.262E-02-1.038E-02
  6.898E+01  1.322E-01  +0.000E+00-0.000E+00
  7.444E+01  1.330E-01  +0.000E+00-0.000E+00
  7.982E+01  7.797E-02  +0.000E+00-0.000E+00
  8.415E+01  8.732E-02  +0.000E+00-0.000E+00
 \END;
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