/*===================================================================*/
 /* NRDF D0327 Data No.10                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,10;
 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,10;
 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,10;
 RSD=128BA'4';
 /*@4@*/
 /*FIG.4-(C)*/
 /* D327                           FIG.4-(C)                       */
 /* SER#=    3            */
 /* XSCALE=LINEAR     YSCALE=LINEAR     */
 /* XMAX= 1.80000000E+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)
          26.808     9.462E-01    4.102E-02
          43.404     1.054E+00    2.564E-02
          60.638     1.095E+00    3.589E-02
          78.510     1.064E+00    2.564E-02
          98.936     1.079E+00    XXXXXXXXX
         116.808     1.044E+00    XXXXXXXXX
         137.234     9.769E-01    XXXXXXXXX
         153.830     9.205E-01    XXXXXXXXX
         171.702     9.000E-01    2.051E-02
         187.659     7.974E-01    XXXXXXXXX
 \END;
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