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 /* NRDF D0363 Data No.25                                             */
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 /* Bibliography                                                      */
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 \\BIB,25;
 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,25;
 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,25;
 EXC-ENGY=1.451MEV;
 DELTA-EXC-ENGY=XMEV;
 J-PI=5/2-;
 /*FIG.9-(D)*/
 /* D363                           FIG.9-(D)                       */
 /* SER#=   18            */
 /* XSCALE=LINEAR     YSCALE=LOG        */
 /* XMAX= 7.00000000E+01   YMAX= 1.00000000E+00 */
 /* XMIN= 0.00000000E+00   YMIN= 9.99999931E-04 */
 /* 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)
           5.945     1.561E+00    6.447E-02
           8.025     1.786E+00    9.904E-02
          10.255     1.459E+00    8.090E-02
          12.187     1.099E+00    6.094E-02
          14.119     7.041E-01    2.908E-02
          16.200     4.160E-01    1.718E-02
          18.280     2.361E-01    9.751E-03
          20.361     1.928E-01    1.069E-02
          22.442     1.902E-01    1.604E-02
          24.374     1.596E-01    6.593E-03
          26.306     1.219E-01    5.034E-03
          28.238     8.467E-02    2.315E-03
          30.467     5.425E-02    4.573E-03
          32.845     4.491E-02    2.490E-03
          34.926     3.619E-02    2.006E-03
          36.560     3.120E-02    8.533E-04
          38.641     2.257E-02    1.251E-03
          40.573     1.819E-02    1.008E-03
          42.803     1.150E-02    8.022E-04
          44.883     1.060E-02    5.878E-04
 \END;
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