/*===================================================================*/
 /* NRDF D0327 Data No.9                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,9;
 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,9;
 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,9;
 RSD=131BA'4';
 /*@4@*/
 /*FIG.4-(B)*/
 /* D327                           FIG.4-(B)                       */
 /* SER#=    5            */
 /* XSCALE=LINEAR     YSCALE=LINEAR     */
 /* XMAX= 1.80000000E+02   YMAX= 1.29999924E+00 */
 /* XMIN= 0.00000000E+00   YMIN= 3.99999976E-01 */
 /* FOLLOWING DATA ARE TAKEN FROM GRAPH */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
           THTL        DATA-REL'3,10'   DELTA-DATA-REL
          (DEG)        (NODIM)        (NODIM)
          25.865     9.618E-01    3.121E-02
          39.589     1.045E+00    XXXXXXXXX
          53.314     1.082E+00    XXXXXXXXX
          68.094     1.050E+00    3.121E-02
          84.985     1.035E+00    XXXXXXXXX
          99.765     1.009E+00    XXXXXXXXX
         116.129     9.410E-01    XXXXXXXXX
         129.853     8.942E-01    XXXXXXXXX
         145.161     8.318E-01    3.641E-02
         158.358     7.486E-01    XXXXXXXXX
 \END;
 /*===================================================================*/