/*===================================================================*/
 /* NRDF D0327 Data No.8                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,8;
 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,8;
 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'53';
 /*@53@*/
 DET-PARTCL=(X);
 SOLID-ANGL=0.16SR'63';
 /*@63@*/
 PHQ=(ANGL-DSTRN'64,65,66,67');
 /*@58@*/
 /*@59@*/
 /*@64@*/
 /*@65@*/
 /*@67@*/
 /*@66@*/
 ANL=(X'68');
 /*@68@*/
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,8;
 RSD=135BA'5';
 /*@5@*/
 /*FIG.4-(A)*/
 /* D327                           FIG.4-(A)                       */
 /* SER#=    7            */
 /* XSCALE=LINEAR     YSCALE=LINEAR     */
 /* XMAX= 1.50000000E+02   YMAX= 1.29999924E+00 */
 /* XMIN= 0.00000000E+00   YMIN= 6.99999988E-01 */
 /* FOLLOWING DATA ARE TAKEN FROM GRAPH */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
         THTL         DATA-REL'3,10'   DELTA-DATA-REL'3,10'
         (DEG)       (NODIM)           (NODIM)
           23.94       9.68E-01     8.03E-02
           35.11       1.07E+00     4.82E-02
           50.53       1.06E+00     XXXXXXXX
           66.49       1.14E+00     XXXXXXXX
           82.45       1.01E+00     XXXXXXXX
           97.87       9.89E-01     2.67E-02
          113.83       9.79E-01     3.21E-02
          129.26       9.57E-01     XXXXXXXX
          142.55       9.79E-01     XXXXXXXX
          157.45       8.82E-01     XXXXXXXX
 \END;
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