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 /* NRDF D0363 Data No.32                                             */
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 /* Bibliography                                                      */
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 \\BIB,32;
 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                                           */
 /*===================================================================*/
 \\EXP,32;
 RCT=208PB(P,D)207PB;
 ENR=>99%;
 CHM=ELM;
 THK-TGT=16.2MG/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,32;
 EXC-ENGY=3.409MEV;
 DELTA-EXC-ENGY=XMEV;
 J-PI=9/2-;
 /*FIG.11-(C)*/
 /* D363                           FIG.11-(C)                      */
 /* SER#=   24            */
 /* XSCALE=LINEAR     YSCALE=LOG        */
 /* XMAX= 7.00000000E+01   YMAX= 1.00000000E+00 */
 /* XMIN= 0.00000000E+00   YMIN= 9.99999791E-03 */
 /* FOLLOWING DATA ARE TAKEN FROM GRAPH */
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 /* Data Table                                                        */
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 \DATA;
        THTC     DSIGMA/DOMEGA
        (DEG)     (MB/SR)
           6.248     2.316E+00
           8.415     2.651E+00
          10.328     2.815E+00
          12.368     1.795E+00
          14.280     1.310E+00
          16.576     2.967E-01
          18.488     4.653E-01
          20.273     3.150E-01
          22.058     2.631E-01
          24.353     3.104E-01
          26.011     1.557E-01
          27.796     1.038E-01
          30.219     7.135E-02
          32.004     5.447E-02
          34.044     4.759E-02
          35.829     3.858E-02
          37.869     2.612E-02
          39.909     1.850E-02
          42.204     1.433E-02
          43.862     1.145E-02
 \END;
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