DARPE: Search Results
 /*===================================================================*/
 /* NRDF D0327 Data No.3                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,3;
 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,3;
 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,3;
 INC-ENGY-LAB=11.5GEV;
 RSD=128BA'4';
 THTL=90DEG;
 /*@4@*/
 /*FIG.3-(C)*/
 /* D327                           FIG.3-(C)                       */
 /* SER#=    1            */
 /* XSCALE=LINEAR     YSCALE=LINEAR     */
 /* XMAX= 1.80000000E+02   YMAX= 2.39999950E-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)
          25.932     1.274E-01    8.044E-03
          28.220     1.502E-01    9.385E-03
          31.271     1.488E-01    9.385E-03
          31.271     1.823E-01    1.206E-02
          46.525     1.676E-01    9.385E-03
          46.525     1.904E-01    1.072E-02
          48.051     2.105E-01    9.385E-03
          52.627     1.971E-01    1.340E-02
          64.068     2.025E-01    9.385E-03
          65.593     2.172E-01    9.385E-03
          71.695     2.051E-01    9.385E-03
          81.610     1.649E-01    8.044E-03
          84.661     1.904E-01    9.385E-03
          84.661     1.810E-01    8.044E-03
          93.051     1.689E-01    9.385E-03
         100.678     1.448E-01    9.385E-03
         104.491     1.327E-01    8.044E-03
         106.780     1.381E-01    9.385E-03
         114.407     1.274E-01    8.044E-03
         121.271     8.983E-02    1.072E-02
         125.847     9.251E-02    9.385E-03
         128.898     7.374E-02    XXXXXXXXX
         137.288     8.313E-02    XXXXXXXXX
         145.678     5.631E-02    XXXXXXXXX
         149.492     3.486E-02    XXXXXXXXX
         154.830     3.486E-02    XXXXXXXXX
         161.695     2.950E-02    XXXXXXXXX
         165.508     1.341E-02    XXXXXXXXX
         172.373     2.681E-03    XXXXXXXXX
         184.576     2.681E-03    XXXXXXXXX
         189.153     1.341E-03    XXXXXXXXX
 \END;
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