/*===================================================================*/
 /* NRDF D1763 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1763;
 TITLE=/Experimental neutron-production double-differential cross
        section for the nuclear reaction by 1.5-GeV pi+ mesons incident
        on iron/;
 PURPOSE=/In this work, the neutron-production double-differential
          cross sections were measured for irons by the use of 1.5-GeV
          pi+ Mesons, and the applicability of the intranuclear
          cascade-evaporation model to this reaction is studied./;
 ATH=(T.NAKAMOTO'1', K.ISHIBASHI'1', N.MATSUFUJI'1', N.SHIGYO'1',
      K.MAEHATA'1', H.ARIMA'1', S.MEIGO'2', H.TAKADA'2', S.CHIBA'2',
      M.NUMAJIRI'3');
 INST-ATH=(2JPNKYU'1', 2JPNJAE'2', 2JPNKEK'3');
      /* '1' Department of Nuclear Engineering */
 REF=NST;
 VLP=34(1997)860;
 RCTS=FE(PIP,N)X;
 PHQS=ENGY-SPEC;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2004-10-13 : Converted, Converted from EXFOR J1763 */
 /* 2002-10-06 : Compiled */
 RTY=SPAL;
 PHQ=ENGY-SPEC;
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2'4';
 /* '4' 4.9cm in diameter and 3.0cm thick */
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN'5';
 /* '5' The pi-2 beam line of the 12GeV proton synchrotron */
 INST-ACC=2JPNKEK;
 INC-ENGY-LAB=1.5GEV;
 POL-PRJ=0%;
 ION-SOURCE=/ Incident pions were generated as secondary beam. The TOF
              of incident particles was measured for separation of pi+
              mesons from protons by the use of a pair of Pilot U
              scintillators. /;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'6',TOF);
 /* '6' Two different sizes (12.7 cm in diameter and 12.7 cm thick,
        5.08 cm in diameter and 5.08 cm thick) of NE213 neutron
        detectors were placed in the directions of 30 degree, 90 degree
        and 150 degree */
 ERS-DET=XKEV'7';
 /* '7' The typical energy resolution is 5.3% at the neutron energy
        of 10 MeV and 15% at 300 MeV */
 EFCN-DET=/ The neutron detection efficiencies were obtained from
            calculation results of SCINFUL [J.K.Dickens, ORNL-6452
            (1988)] and CECIL [R.A.Cecil et al., Nucl. Instrum.
            Methods, 161 (1979) 439] codes. The uncertainty of the
            neutron detection efficiencies were determined to be 10% in
            the neutron energy region below 80 MeV, while there are set
            at 15% above 80 MeV. /;
 ANL=MONTE-MTHD'8';
 /* '8' High Energy Transport Code (HETC) [K.C.Chandler,
        T.W.Armstrong, CCC-178 (1977), W.A.Coleman, T.W.Armstrong,
        ORNL-4606 (1970)] */
 /* Experimental Method:
    - Time-of-flight
 RCT=FE(PIP,N)X;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 INC-ENGY-LAB=1.5GEV;
 EMT=N;
 THTL=90DEG;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 ENGY-EMT-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
 (MEV) (MB/SR/MEV) (MB/SR/MEV)
   +1.268E+00 +2.616E+01 +5.290E+00-8.061E+00
   +1.809E+00 +2.594E+01 +8.256E+00-7.148E+00
   +2.530E+00 +2.242E+01 +5.804E+00-5.412E+00
   +3.537E+00 +1.340E+01 +2.711E+00-3.236E+00
   +4.571E+00 +1.108E+01 +1.641E+00-3.054E+00
   +5.566E+00 +8.764E+00 +1.298E+00-2.414E+00
   +6.915E+00 +7.594E+00 +1.966E+00-1.833E+00
   +9.113E+00 +5.724E+00 +8.479E-01-1.177E+00
   +1.273E+01 +3.268E+00 +4.841E-01-9.006E-01
   +1.745E+01 +1.702E+00 +4.408E-01-4.110E-01
   +2.538E+01 +1.404E+00 +4.468E-01-3.868E-01
   +3.621E+01 +1.158E+00 +2.998E-01-2.795E-01
   +4.587E+01 +8.737E-01 +2.262E-01-2.109E-01
   +5.698E+01 +7.231E-01 +1.872E-01-1.745E-01
   +6.938E+01 +4.980E-01 +1.007E-01-1.372E-01
   +9.143E+01 +3.930E-01 +1.017E-01-8.083E-02
   +1.252E+02 +2.047E-01 +5.301E-02-6.309E-02
   +1.751E+02 +1.224E-01 +3.896E-02-4.153E-02
   +2.495E+02 +4.210E-02 +1.601E-02-1.553E-02
 \END;
 /*===================================================================*/