/*===================================================================*/
 /* NRDF D0178 Data No.24                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,24;
 D#=D178;
 TITLE=/'BACKWARD' PRODUCTION OF PROTONS,DEUTERONS,TRITONS,3HE,4HE AND
         PIONS IN THE INTERACTION OF 400GEV PROTONS WITH NUCLEI/;
 PURPOSE=/THE PRODUCTION OF PARTICLES IN INTERACTIONS WITH NUCLEI, IN
          KINEMATIC REGIONS NOT ACCESIBLE IN INTERACTIONS WITH FREE
          STATIONARY NUCLEONS IS BELIEVED TO BE SENSITIVE TO THE HIGH
          MOMENTUM PART OF THE NUCLEAR WAVE FUNCTION OR TO COLLECTIVE
          BEHAVIOR IN NUCLEI.   IN ORDER TO PUT  THE VARIOUS THEORIES
          TO A TEST OVER A WIDE RANGE OF ENERGIES, AND  ON THE
          SUPPOSITION THAT SIMILAR HIGH MOMENTUM FEATURES OF THE
          STRUCTURE OF NUCLEI OUGHT TO BE EXTRACTABLE WITH BOTH VERY
          LOW AND VERY HIGH ENERGY PROBES, WE HAVE CHOSEN TO DIRECT OUR
          ATTENTION TO A STUDY OF THESE CROSS SECTIONS  AT THE HIGHEST
          AVAILABLE ENERGIES, 400GEV PROTONS AT FERMMI-LAB./;
 ATH=(Y.D.BAYUKOV'1',V.I.EFREMENKO'1',S.FRANKEL'1',W.FRATI'1',
      M.GAZZALY'1',G.A.LEKSIN'1',N.A.NIKIFOROV'1',C.F.PERDRISAT'1',
      V.I.TCHISTILIN'1',Y.M.ZAITSEV'1');
 INST-ATH=(X'1');
 /*@3@*/
 REF=PL/B;
 VLP=85(1979)315;
 RCTS=(6LI(P,P)X,181TA(P,P)X,181TA(P,D)X,181TA(P,T)X,181TA(P,3HE)X,181TA
 (P,4HE)X,181TA(P,PIP)X,181TA(P,PIN)X,9BE(P,PIP)X,9BE(P,P)X,9BE(P,D)X,9B
 E(P,T)X,C(P,PIP)X,C(P,P)X,C(P,D)X,C(P,T)X,AL(P,PIP)X,AL(P,P)X,AL(P,D)X,
 AL(P,T)X,CU(P,PIP)X,CU(P,PIP)X,CU(P,P)X,CU(P,D)X,CU(P,T)X);
 /*@4@*/
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,24;
 RCT=9BE(P,T)X;
 /*@4@*/
 THK-TGT=XMG/CM**2;
 POL-TGT=NO;
 ALGN-TGT=NO;
 RCT=C(P,T)X;
 /*@4@*/
 THK-TGT=XMG/CM**2;
 POL-TGT=NO;
 ALGN-TGT=NO;
 RCT=AL(P,T)X;
 /*@4@*/
 THK-TGT=XMG/CM**2;
 POL-TGT=NO;
 ALGN-TGT=NO;
 RCT=CU(P,T)X;
 /*@4@*/
 THK-TGT=XMG/CM**2;
 POL-TGT=NO;
 ALGN-TGT=NO;
 INST-ACC=1USANAL;
 INC-ENGY-LAB-RANGE=(400GEV);
 DELTA-INC-ENGY=XKEV;
 ERS-PRJ=XKEV;
 BEAM-INTNSTY=XUA;
 POL-PRJ=NO;
 DET-SYS=(MAG+X);
 /*@5@*/
 SOLID-ANGL=1.13MSR;
 ERS-DET=XKEV;
 PHQ=(XSECTN,ENGY-SPEC,DSIGMA/DOMEGA/DE'1',XSECTN-RATIO);
 /*@6@*/
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,24;
 INC-ENGY-LAB=400GEV;
 THTL=160DEG;
 /*FIG.5-(H)*/
 /* D178                           FIG 5-(H)                       */
 /* SER#=   24            */
 /* XSCALE=LOG        YSCALE=LOG        */
 /* XMAX= 1.81000000E+02   YMAX= 1.00000000E+01 */
 /* XMIN= 6.00000000E+00   YMIN= 1.00000000E+00 */
 /* FOLLOWING DATA ARE TAKEN FROM GRAPH */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
            A'1'       DATA2'2'   DELTA-DATA2'2'
          (NODIM)       (NODIM)    (NODIM)
            6.08       1.03E+00     XXXXXXXX
            8.92       2.26E+00     3.65E-01
           11.89       4.49E+00     XXXXXXXX
           26.66       1.22E+01     XXXXXXXX
           63.12       3.32E+01     XXXXXXXX
          178.54       1.03E+02     XXXXXXXX
 \END;
 /*===================================================================*/