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 /* NRDF D0363 Data No.31                                             */
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 /* Bibliography                                                      */
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 \\BIB,31;
 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,31;
 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,31;
 EXC-ENGY=2.340MEV;
 DELTA-EXC-ENGY=XMEV;
 J-PI=7/2-;
 /*FIG.11-(B)*/
 /* D363                           FIG.11-(B)                      */
 /* SER#=   23            */
 /* XSCALE=LINEAR     YSCALE=LOG        */
 /* XMAX= 7.00000000E+01   YMAX= 1.00000000E+01 */
 /* XMIN= 0.00000000E+00   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)
           6.467     3.186E+00    XXXXXXXXX
           8.496     2.666E+00    XXXXXXXXX
          10.272     1.707E+00    XXXXXXXXX
          12.554     7.430E-01    XXXXXXXXX
          14.456     4.163E-01    XXXXXXXXX
          16.232     3.588E-01    XXXXXXXXX
          18.388     2.871E-01    XXXXXXXXX
          20.543     2.040E-01    XXXXXXXXX
          22.446     1.471E-01    XXXXXXXXX
          24.475     1.030E-01    XXXXXXXXX
          26.630     9.564E-02    XXXXXXXXX
          28.152     8.492E-02    XXXXXXXXX
          30.181     5.686E-02    XXXXXXXXX
          32.210     3.865E-02    XXXXXXXXX
          34.239     3.483E-02    XXXXXXXXX
          36.141     3.186E-02    XXXXXXXXX
          38.170     2.549E-02    XXXXXXXXX
          42.228     1.160E-02    XXXXXXXXX
          44.257     9.012E-03    1.289E-03
 \END;
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