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 /* NRDF D0363 Data No.19                                             */
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 /* Bibliography                                                      */
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 \\BIB,19;
 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,19;
 RCT=58NI(P,D)57NI;
 ENR=>99%;
 CHM=ELM;
 THK-TGT=11.1MG/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,19;
 EXC-ENGY=5.784MEV;
 DELTA-EXC-ENGY=XMEV;
 /*FIG.7-(I)*/
 /* D363                           FIG.7-(I)                       */
 /* SER#=   13            */
 /* XSCALE=LINEAR     YSCALE=LOG        */
 /* XMAX= 7.00000000E+01   YMAX= 9.99999642E-02 */
 /* XMIN= 9.99999791E-03   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)
           5.973     5.688E-02    1.260E-02
           8.327     8.804E-02    1.015E-02
          10.524     1.605E-01    XXXXXXXXX
          12.407     1.244E-01    XXXXXXXXX
          14.134     5.899E-02    5.620E-03
          16.174     1.479E-02    2.318E-03
          18.371     1.908E-02    3.396E-03
          20.568     8.884E-03    2.578E-03
          22.294     2.090E-02    3.276E-03
          24.491     1.807E-02    XXXXXXXXX
          26.060     1.452E-02    1.675E-03
          28.100     1.066E-02    1.229E-03
          30.297     6.640E-03    1.181E-03
          32.651     6.761E-03    1.203E-03
          34.220     5.053E-03    7.920E-04
          36.103     4.785E-03    3.613E-04
          38.144     1.695E-03    5.731E-04
          40.341     6.062E-03    8.237E-04
          42.381     1.997E-03    6.269E-04
          44.421     1.413E-03    5.125E-04
          46.147     2.187E-03    4.366E-04
 \END;
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