/*===================================================================*/
 /* NRDF D0152 Data No.4                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,4;
 D#=D152;
 TITLE=/(P,D) REACTIONS AT 52 MEV.I.58NI(P,D)57NI (EXPERIMENTAL)/;
 PURPOSE=/TO TEST THE VALIDITY OF CURRENT REACTION THEORIES,(P,D)ANGULAR
          DISTRIBUTION HAVE BEEN TAKEN AT THE INCIDENT ENERGY OF 52MEV,
          THE HIGHEST ENERGY SO FAR STUDIED,OVER A WIDE RANGE OF ANGLES
          AND IN SMALL STEPS'D'/;
 ATH=(H.OHNUMA'C',T.SUEHIRO'A,C',M.SEKIGUCHI'C',S.YAMADA'B,C');
 INST-ATH=(2JPNINS'C');
 /* 'A' PRESENT ADRESS:TOHOKU INSTITUTE OF TECHNOLOGY */
 /* 'B' PRESENT ADRESS: TOKYO INSTITUTE OF TECHNOLOGY */
 REF=JPJ;
 VLP=36(1974)1236;
 RCTS=(58NI(P,D)57NI);
 /* 'D'THE 58NI(P,D)REACTION,WHICH WE BELIEVE REQUIRE ANALYSIS FROM
    VARIOUS ASPECTS. BRIET DESCRIPTION OF ANALYSIS AND SPECTIOSCOPIC
    INFORMATION OBTAINED ARE ALSO GIVEN. DETAILS OF THE ANALYSIS WE HAVE
    DONE SO FAR WILL BE GIVEN IN A SUBSEQUENT PAPER: H.OHNUMA ET AL.,
    J .PHYS.SOC.JAPAN 36(1974)1245 */
 /*===================================================================*/
 /* Experimental Conditions                                           */
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 \\EXP,4;
 RCT=58NI(P,D)57NI;
 CHM=ELM;
 THK-TGT=2.7MG/CM**2;
 BAC=SELF;
 ACC=(SYNCYC);
 INST-ACC=2JPNINS;
 INC-ENGY-RANGE=(51.93MEV);
 DET-PARTCL=(D);
 DET-SYS=(D);
 DET-SYS=(MAG+PROP-CNTR);
 ERS-DET=70KEV;
 ANL=(OPT-MODEL,DWBA);
 PHQ=(ANGL-DSTRN);
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 /* Descriptive Parameters                                            */
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 \\DATA,4;
 INC-ENGY=51.93MEV;
 THTC=5.8[110.3DEG;
 EXC-ENGY=2.56MEV;
 J-PI=7/2-;
 TRANSF-L=[3;
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (MB/SR) (MB/SR)
   6.0     3.43      0.04
   8.0     2.86      0.04
  10.6     2.57      0.04
  13.1     2.61      0.04
  15.7     2.60      0.03
  18.3     2.55      0.03
  20.8     2.35      0.03
  23.4     1.93      0.02
  26.0     1.40      0.02
  28.5     1.01      0.02
  31.1     0.84      0.01
  33.7     0.78      0.01
  36.2     0.82      0.01
  38.8     0.77      0.01
  41.3     0.72      0.01
  43.9     0.60      0.01
  46.4     0.46      0.01
  49.0     0.37      0.01
  51.5     0.34      0.01
  54.1     0.35      0.01
  56.6     0.35      0.01
  59.1     0.32      0.01
  61.7     0.29      0.01
  64.2     0.24      0.01
  66.7     0.188     0.005
  69.3     0.156     0.005
  71.8     0.145     0.004
  74.3     0.144     0.004
  76.8     0.136     0.004
  79.4     0.140     0.004
  81.9     0.124     0.004
  86.9     0.097     0.004
  91.9     0.070     0.003
  96.9     0.059     0.003
 101.9     0.052     0.003
 106.8     0.039     0.002
 111.8     0.028     0.002
 \END;
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