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 /* NRDF D0152 Data No.14                                             */
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 /* Bibliography                                                      */
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 \\BIB,14;
 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 */
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 /* Experimental Conditions                                           */
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 \\EXP,14;
 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,14;
 INC-ENGY=51.93MEV;
 THTC=5.8[110.3DEG;
 EXC-ENGY=6.02MEV;
 J-PI=3/2+;
 TRANSF-L=[2;
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 /* Data Table                                                        */
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 \DATA;
 THTC      DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG)     (MB/SR)       (MB/SR)
   6.0     0.69          0.02
   8.0     0.67          0.02
  10.6     0.64          0.02
  13.1     0.59          0.02
  15.7     0.52          0.01
  18.3     0.42          0.01
  20.8     0.33          0.01
  23.4     0.26          0.01
  26.0     0.23          0.01
  28.5     0.23          0.01
  31.1     0.21          0.01
  33.7     0.19          0.01
  36.2     0.18          0.01
  38.8     0.135         0.005
  41.3     0.104         0.004
  43.9     0.089         0.003
  46.4     0.076         0.003
  49.0     0.081         0.003
  51.5     0.084         0.003
  54.1     0.085         0.003
  56.6     0.070         0.003
  59.1     0.067         0.003
  61.7     0.052         0.003
  66.7     0.037         0.002
  69.3     0.034         0.002
  71.8     0.034         0.002
  74.3     0.031         0.002
  76.8     0.031         0.002
  79.4     0.029         0.002
  81.9     0.024         0.002
  86.9     0.020         0.002
  91.9     0.014         0.0014
  96.9     0.013         0.0014
 101.9     0.0099        0.0012
 106.8     0.0090        0.0011
 111.8     0.0074        0.0010
 \END;
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