/*===================================================================*/
 /* NRDF D1833 Data No.4                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,4;
 D#=D1833;
 TITLE=/ Neutron-production double-differential cross sections of
         iron and lead by 0.8 and 1.5 GeV protons in the most-forward
         direction /;
 ATH=(D.SATOH'1', N.SHIGYO'1', K.ISHIBASHI'1', Y.TAKAYAMA'1',
      S.ISHIMOTO'1', Y.IWAMOTO'1', H.TENZOU'1', T.NAKAMOTO'2',
      M.NUMAJIRI'2', S.MEIGO'3');
 INST-ATH=(2JPNKYU'1', 2JPNKEK'2', 2JPNJAE'3');
      /* '1' Department of Applied Quantum Physics and Nuclear
              Engineering */
 REF=NST;
 VLP=40(2003)283;
 /* Secondary reference 
    - NSTS, 4(2004)14 (N.Shigyo et al., Preliminary data given)
 RCTS=(FE(P,N)X, PB(P,N)X);
 PHQS=ENGY-SPEC;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,4;
 /* 2003-08-12 : Compiled+Checked, Im. */
 /* 2005-02-08 : Received, On. Received by e-mail from N.Shigyo */
 /* 2010-02-23 : Altered, Nf. REFERENCE: NSTS added */
 PHQ=ENGY-SPEC;
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN'5';
 /* '5' 12-GeV PS */
 INST-ACC=2JPNKEK;
 POL-PRJ=0%;
 ION-SOURCE=/ Spallation (Incident protons were generated as secondary
              particles from an internal target which was placed in the
              12-GeV PS main ring.) /;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'6',TOF'7');
 /* '6' NE102A scintillator was mounted as a veto detector to
        reject the charged particle events. */
 /* '7' The high-resolution TOF measurement of 0-degree neutron was
        done. This provides a higher detection efficiency and uses a
        simpler data analysis than the recoil proton method. */
 ERS-DET=150MEV'8';
 /* '8' for 800 MeV protons */
 EFCN-DET=/ The neutron detection efficiencies were obtained from
            calculation results of SCINFUL-QMD [D.Satoh, et al., IEEE
            Trans. Nucl. Sci., 48, 1165 (2001); D.Satoh, et al., J.
            Nucl Sci. Technol., Supplement 2, 657 (2002)]. /;
 ANL=(INCASC'9',INCASC'10');
 /* '9' NMTC/JAM[K.Niita et al., JAERI-Data/Code 2001-007, JAERI,
        (2001).] */
 /* '10' JQMD[K.Niita et al., JAERI-Data/Code 99-042, JAERI,
         (1999).] */
 /* 2010-02-23 : Altered, Nf. STATUS: Free text revised */
 RCT=PB(P,N)X;
 THK-TGT=XMG/CM**2'21';
 /* '21' 20 mm */
 INC-ENGY-LAB-RANGE=1.5GEV;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,4;
 SYS-ERR=15%'11';
 /* '11' Ambiguity of neutron detection efficiency */
 INC-ENGY-LAB=1.5GEV;
 THTL=0DEG;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 ENGY-EMT-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE'22' FLAG'23'
 (MEV) (MB/SR/MEV) (MB/SR/MEV) (NODIM)
 425.00 2.2413 +-0.33620 1.
 475.00 1.7919 +-0.26879 1.
 525.00 1.7385 +-0.26078 1.
 575.00 1.6012 +-0.24018 1.
 625.00 1.5580 +-0.23370 X
 675.00 1.4858 +-0.22287 X
 750.00 1.5872 +-0.23809 X
 850.00 2.1147 +-0.33220 X
 950.00 2.2281 +-0.31922 X
 1075.0 1.4676 +-0.26550 X
 1225.0 0.99453 +-0.20120 X
 1375.0 0.50310 +-0.11109 X
 1525.0 0.39179 +-0.095850 X
 \END;
 /*===================================================================*/