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 /* NRDF D0363 Data No.23                                             */
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 /* Bibliography                                                      */
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 \\BIB,23;
 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,23;
 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,23;
 EXC-ENGY=0.588MEV;
 DELTA-EXC-ENGY=XMEV;
 J-PI=1/2-;
 /*FIG.9-(B)*/
 /* D363                           FIG.9-(B)                       */
 /* SER#=   16            */
 /* XSCALE=LINEAR     YSCALE=LOG        */
 /* XMAX= 7.00000000E+01   YMAX= 1.00000000E+00 */
 /* XMIN= 9.99999791E-03   YMIN= 9.99999791E-03 */
 /* 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)
           6.386     6.629E-01    3.735E-02
           8.462     4.275E-01    3.032E-02
          10.242     2.610E-01    1.095E-02
          12.021     1.754E-01    1.503E-02
          14.394     1.086E-01    9.305E-03
          16.321     6.720E-02    8.822E-03
          18.397     4.455E-02    5.848E-03
          20.473     3.992E-02    4.626E-03
          22.401     4.334E-02    3.714E-03
          24.625     2.953E-02    3.421E-03
          26.553     2.307E-02    1.636E-03
          28.777     1.262E-02    2.054E-03
          30.705     7.296E-03    1.304E-03
          32.336     6.190E-03    2.410E-03
          34.560     7.397E-03    9.710E-04
          36.784     5.039E-03    9.009E-04
          38.860     5.623E-03    1.005E-03
          40.936     3.938E-03    5.784E-04
 \END;
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