/*===================================================================*/
 /* NRDF D0082 Data No.12                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,12;
 D#=D82;
 TITLE=/J DEPENDENCE OF THE ANALYZING POWER FOR (P,ALPHA) REACTIONS/;
 ATH=(Y.TAGISHI'1',K.KATORI'1',M.SASAGASE'1',M.SATO'1',T.MIKUMO'1');
 INST-ATH=(2JPNTSU'1');
 REF=PR/C;
 VLP=19(1979)2420;
 RCTS=(40CA(P,ALPHA)37K,60NI(P,ALPHA)57CO,62NI(P,ALPHA)59CO);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,12;
 RCT=62NI(P,ALPHA)59CO;
 ENR=98.7%;
 CHM=ELM;
 THK-TGT=0.280MG/CM**2;
 BAC=SELF;
 POL-TGT=NO;
 ALGN-TGT=NO;
 ACC=(VDGT);
 INST-ACC=2JPNTSU;
 INC-ENGY-LAB-RANGE=(22.0MEV);
 BEAM-INTNSTY=100NA;
 POL-PRJ=YES'1';
 /*@3@*/
 DET-PARTCL=(ALPHA);
 DET-SYS=(MAG+PS-SI);
 SOLID-ANGL=2.0MSR;
 ERS-DET=35[50KEV;
 ANL=(OPT-MODEL,DWBA'2');
 /*@4@*/
 PHQ=(DSIGMA/DOMEGA,ANALPW,OPT-POTL-PARA);
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,12;
 INC-ENGY-LAB=22.0MEV;
 EXC-ENGY=3.16MEV;
 J-PI=3/2+;
 /*FIG.3-(3)*/
 /* D408                           FIG.3-(3)                       */
 /* SER#=   13            */
 /* XSCALE=LINEAR     YSCALE=LINEAR     */
 /* XMAX= 8.00000000E+01   YMAX= 1.00000000E+00 */
 /* XMIN= 0.00000000E+00   YMIN=-1.00000000E+00 */
 /* FOLLOWING DATA ARE TAKEN FROM GRAPH */
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
           THTC           ANALPW     DELTA-ANALPW
            (DEG)         (NODIM)         (NODIM)
          10.377    -1.418E-01    +3.402E-02-2.646E-02
          15.660    -2.023E-01    +3.024E-02-3.024E-02
          21.132    -1.607E-01    +3.402E-02-3.780E-02
          26.604     1.153E-01    +4.158E-02-3.402E-02
          31.321     3.459E-01    +3.024E-02-4.158E-02
          37.170     5.728E-01    +3.402E-02-3.024E-02
          41.887     5.841E-01    +3.024E-02-3.402E-02
          46.981     5.161E-01    +2.646E-02-2.268E-02
          52.075     5.577E-01    +5.293E-02-6.427E-02
          56.981     6.446E-01    +3.024E-02-7.183E-02
          62.075     7.505E-01    +4.914E-02-6.805E-02
          66.792     6.181E-01    +4.914E-02-7.183E-02
          71.887     3.837E-01    +6.427E-02-5.671E-02
          76.981     1.267E-01    +8.695E-02-1.020E-01
          82.453     3.270E-01    +1.172E-01-1.323E-01
 \END;
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