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 /* NRDF D0363 Data No.22                                             */
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 /* Bibliography                                                      */
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 \\BIB,22;
 D#=D363;
 TITLE=/A STUDY OF THE 58NI,90ZR AND 208PB(P,D) REACTIONS AT 121 MEV/;
 PURPOSE=/IN ORDER TO INVESTIGATE THE EXTENT TO WHICH THE DISTORTED WAVE
          METHOD CAN BE EXTENDED TO HIGHER BOMBARDING ENERGIES, THE
          58NI, 9/ZR AND 208PB(P,D) REACTIONS WERE STUDIED AT 121 MEV.
          THE MAJOR EMPHASIS IN THE PRESENT WAS TO STUDY THE LOW-LYING
          STATES THAT ARE STRONGLY EXCITED AND HENCE HAVE SPECTROSCOPIC
          FACTORS THAT WERE RATHER WELL DETERMINDED IN EARLIER WORK DONE
          AT LOWER BOMBARDING ENERGIES./;
 ATH=(R.E.ANDERSON'1',J.J.KRAUSHAAR'1',J.R.SHEPARD'1',J.R.COMFORT'2');
 INST-ATH=(1USACLU'1',1USAINU'2');
 REF=NP/A;
 VLP=311(1978)93;
 RCTS=(58NI(P,D)57NI,90ZR(P,D)89ZR,208PB(P,D)207PB);
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 /* Experimental Conditions                                           */
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 \\EXP,22;
 RCT=90ZR(P,D)89ZR;
 ENR=98%;
 CHM=ELM;
 THK-TGT=15.0MG/CM**2;
 BAC=SELF;
 POL-TGT=NO;
 ALGN-TGT=NO;
 ACC=(CYC);
 INST-ACC=1USAINU;
 INC-ENGY-LAB-RANGE=(121.2MEV);
 DELTA-INC-ENGY-LAB=XKEV;
 ERS-PRJ=XKEV;
 BEAM-INTNSTY=XUA;
 POL-PRJ=NO;
 DET-SYS=(MAG+PS-PC+PLST-SCT);
 SOLID-ANGL=2.55MSR;
 ERS-DET=125KEV;
 ANL=(OPT-MODEL,CC,DWBA);
 PHQ=(XSECTN,ANGL-DSTRN,DSIGMA/DOMEGA,OPT-POTL-PARA,SPEC-FCTR);
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 /* Descriptive Parameters                                            */
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 \\DATA,22;
 EXC-ENGY=0.0MEV;
 DELTA-EXC-ENGY=XMEV;
 J-PI=9/2+;
 /*FIG.9-(A)*/
 /* D363                           FIG.9-(A)                       */
 /* SER#=   15            */
 /* XSCALE=LINEAR     YSCALE=LOG        */
 /* XMAX= 7.00000000E+01   YMAX= 1.00000000E+01 */
 /* XMIN= 9.99999791E-03   YMIN= 9.99999642E-02 */
 /* FOLLOWING DATA ARE TAKEN FROM GRAPH */
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 /* Data Table                                                        */
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 \DATA;
        THTC     DSIGMA/DOMEGA    DELTA-DSIGMA/DOMEGA
       (DEG)         (MB/SR)           (MB/SR)
           6.507     5.913E+00    3.362E-01
           8.279     6.604E+00    2.797E-01
          10.346     6.696E+00    2.836E-01
          12.561     6.163E+00    2.610E-01
          13.742     4.805E+00    2.035E-01
          16.548     3.262E+00    1.381E-01
          18.467     2.067E+00    8.755E-02
          20.830     1.365E+00    5.782E-02
          22.602     9.931E-01    5.648E-02
          24.669     8.648E-01    2.425E-02
          27.031     7.326E-01    2.054E-02
          28.656     5.633E-01    2.386E-02
          30.723     4.272E-01    1.809E-02
          32.790     3.331E-01    1.894E-02
          34.857     2.744E-01    1.162E-02
          36.629     2.293E-01    1.304E-02
          38.696     1.863E-01    7.892E-03
          40.911     1.413E-01    8.036E-03
          43.274     9.727E-02    4.120E-03
          45.046     7.584E-02    4.313E-03
 \END;
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