DARPE: Search Results
 /*===================================================================*/
 /* NRDF D0327 Data No.2                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D327;
 TITLE=/DIFFERENTIAL RANGES AND ANGULAR DISTRIBUTIONS OF BA FRAGMENTS
        FROM THE INTERACTION OF 238U WITH 11.5-GEV PROTONS/;
 PURPOSE=/AS SHOWN IN FIGURE OF Z-DEPENDENCE OF THE ISOBARIC
          THICK-TARGET RANGES AND CROSS SECTIONS OF A=131 NUCLIDES FROM
          THE INTERACTION OF 238U WITH 11.5-GEV PROTONS, THE RANGE OF
          131BA LIES MIDWAY BETWEEN THE FISSION AND DEEP SPALLATION
          RANGES. THE MOST OBVIOUS EXPLANATION OF THIS FACT IS THAT AT
          A=131 THE TRANSITION BETWEEN THESE PROCESSES OCCURS BETWEEN
          Z=55 AND 57, WITH COMPARABLE CONTRIBUTIONS OCURRING AT Z=56.
          THIS EXPLABATUIB ASSUMES THAT ONLY TWO MECHANISMES ARE
          OPERATIVE AND THIS IS FAR FROM CERTAIN.  THE RESULTS PRESENTED
          HERE PERMIT A DETERMINATION OF HOW THE ANGULAR DISTRIBUTION
          AND THE WIDTH OF THE SPECTRUM, QUANTITIES THAT CANNOT BE
          INFERRED FROM THICK-TARGET RECOIL STUDIES, CHANGE AS THE
          TRANSITION BETWEEN MECHANISMS IS ACCHIEVED./;
 ATH=(N.T.PORILE'1',S.PANDIAN'1',H.KLONK'1',C.R.RUDY'1',E.P.STEINBERG'2'
 INST-ATH=(1USAPUR'1',1USAANL'2');
 REF=PR/C;
 VLP=19(1979)1832;
 RCTS=(238U(P,X)128BA,238U(P,X)131LA,238U(P,X)131BA,238U(P,X)135BA,
       238U(P,X)140BA);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 RCT=(238U(P,X)128BA,238U(P,X)131LA,238U(P,X)131BA,238U(P,X)135BA,
      238U(P,X)140BA);
 CHM=UF4;
 THK-TGT=100[300MU-M;
 BAC=AL;
 THK-BAC=20MU-M;
 ACC=(SYN);
 INST-ACC=1USAANL;
 INC-ENGY-RANGE=(11.5GEV'55');
 /*@55@*/
 DELTA-INC-ENGY=XKEV;
 ERS-PRJ=XKEV;
 BEAM-INTNSTY=XUA;
 POL-PRJ=NO;
 DET-PARTCL=(GAMMA);
 DET-SYS=(GE(LI));
 /*@56@*/
 /*@57@*/
 BAC=X'54';
 DET-PARTCL=(X);
 PHQ=(Z-DSTRN,X'60');
 /*@60@*/
 /*@61@*/
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
 INC-ENGY-LAB=11.5GEV;
 RSD=131BA'4';
 THTL=90DEG;
 /*@4@*/
 /*FIG.3-(B)*/
 /* D327                           FIG.3-(B)                       */
 /* SER#=    1            */
 /* XSCALE=LINEAR     YSCALE=LINEAR     */
 /* XMAX= 1.80000000E+02   YMAX= 1.59999967E-01 */
 /* XMIN= 0.00000000E+00   YMIN= 0.00000000E+00 */
 /* FOLLOWING DATA ARE TAKEN FROM GRAPH */
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
           DATA'1'      DATA-REL'3'   DELTA-DATA-REL'3'
           (UNIT'2')      (NODIM)       (NODIM)
          25.618     1.264E-01    9.411E-03
          26.966     1.345E-01    9.411E-03
          26.292     1.439E-01    9.411E-03
          28.989     1.667E-01    1.478E-02
          41.123     1.439E-01    9.411E-03
          41.798     1.734E-01    1.210E-02
          42.472     1.815E-01    1.882E-02
          46.517     1.748E-01    1.075E-02
          55.955     1.909E-01    1.075E-02
          57.977     1.748E-01    1.344E-02
          60.000     1.963E-01    1.075E-02
          64.045     1.909E-01    1.075E-02
          72.809     1.371E-01    1.075E-02
          74.831     1.573E-01    1.210E-02
          75.505     1.775E-01    8.067E-03
          80.899     1.533E-01    1.075E-02
          88.314     1.466E-01    8.067E-03
          92.359     1.385E-01    9.411E-03
          91.685     1.345E-01    6.722E-03
         101.123     1.345E-01    9.411E-03
         106.517     1.089E-01    9.411E-03
         112.584     1.264E-01    1.075E-02
         113.258     1.062E-01    6.722E-03
         120.000     1.264E-01    6.722E-03
         126.741     1.008E-01    8.067E-03
         131.461     8.336E-02    XXXXXXXXX
         132.809     6.723E-02    9.411E-03
         140.899     5.647E-02    XXXXXXXXX
         144.944     4.034E-02    XXXXXXXXX
         151.685     2.017E-02    XXXXXXXXX
         155.056     2.017E-02    XXXXXXXXX
         161.124     6.723E-03    XXXXXXXXX
 \END;
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