/* 2006-11-22 File is generated by HENDEL. */
 \\BIB,1[3;
 D#=D1811;
 TITLE=/ Possible contribution of a highly excited collective state
         to proton-nucleus multistep interactions at 300 MeV /;
 PURPOSE=/ To achieve a more comprehensive understanding of
           spallation reactions /;
 ATH=(Y.UOZUMI'1', J.TANAKA'1', F.SAIHO'1', S.HOHARA'1', CAO BIN'1',
      S.AOKI'1', G.WAKABAYASHI'1', M.MATOBA'1', T.MAKI'2', M.NAKANO'2',
      N.KOORI'3');
 INST-ATH=(2JPNKYU'1', 2JPNKIT'2', 2JPNTKS'3');
      /* '1' Department of Nuclear Engineering */
      /* '3' Faculty of Integrated Arts and Sciences */
 REF=PR/C;
 VLP=64(2001)011601;
 RCTS=12C(P,P)12C;
 PHQS=ENGY-SPEC'4';
 /* '4' Double differential cross section */

 \\EXP,1[3;
 /* 2003-09-21 : Compiled, Kc + On */
 RTY=INEL-SCATT;
 PHQ=ENGY-SPEC'5';
 /* '5' Double differential cross section */
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB=300MEV;
 POL-PRJ=0%;
 DET-PARTCL=P;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=SCT'6';
 /* '6' GSO scintillation crystal [K. Anami et al., Nucl. Instrum.
        Methods Phys. Res. A404(1998)327, H. Yoshida et al., Nucl.
        Instrum. Methods Phys. Res. A411(1998)46] */
 ANL=(INCASC'7',INCASC'8');
 /* '7' Quantum molecular dynamics (QMD) [J. Aichelin, Phys. Rep.
        202(1991)233] */
 /* '8' Intranuclear cascade model (INC) [H.W. Bertini et al.,
        Phys. Rev. 131(1963)1801, Y. Yariv and Z. Fraenkel, Phys. Rev.
        C20(1979)2227] */


 \\DATA,1[3;
 INC-ENGY-LAB=300MEV;
 NORM=/ The experiments were calibrated by pp elastic scattering using
        a CH2 target. /;

 \\EXP,1;
 /* 2006-09-14 : Altered, At. Re-digitized */
 RCT=12C(P,P)12C;

 \\DATA,1;
 THTL=30DEG;
 \DATA;
 ENGY-EMT-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
 (MEV) (MB/SR/MEV) (MB/SR/MEV)
 4.037E+01 3.111E-01 +-3.746E-02
 5.058E+01 3.257E-01 +-3.330E-02
 6.078E+01 3.403E-01 +-3.954E-02
 7.054E+01 3.444E-01 +-3.746E-02
 8.087E+01 3.409E-01 +-3.267E-02
 9.051E+01 3.673E-01 +-3.538E-02
 1.008E+02 3.721E-01 +-3.269E-02
 1.110E+02 3.866E-01 +-3.275E-02
 1.207E+02 4.027E-01 +-3.122E-02
 1.304E+02 4.277E-01 +-3.122E-02
 1.408E+02 4.636E-01 +-3.068E-02
 1.504E+02 4.901E-01 +-3.330E-02
 1.606E+02 5.172E-01 +-3.538E-02
 1.704E+02 5.421E-01 +-3.538E-02
 1.806E+02 5.900E-01 +-3.122E-02
 1.903E+02 6.004E-01 +-3.122E-02
 2.003E+02 6.195E-01 +-2.878E-02
 2.105E+02 6.112E-01 +-3.084E-02
 2.207E+02 6.008E-01 +-3.500E-02
 2.303E+02 6.004E-01 +-2.914E-02
 2.405E+02 5.817E-01 +-3.122E-02
 2.504E+02 4.178E-01 +-6.399E-02
 2.604E+02 3.465E-01 +-8.533E-02
 2.702E+02 1.426E-01 +-1.103E-01
 2.800E+02 6.860E-02 +-1.197E-01
 \END;
 /* Data scanned from Fig.1, p011601-2 in reference */

 \\EXP,2;
 /* 2006-09-14 : Altered, At. Re-digitized */
 RCT=12C(P,P)12C;

 \\DATA,2;
 THTL=40DEG;
 \DATA;
 ENGY-EMT-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
 (MEV) (MB/SR/MEV) (MB/SR/MEV)
 5.011E+01 2.443E-01 +-3.336E-02
 6.075E+01 2.527E-01 +-3.128E-02
 7.095E+01 2.693E-01 +-3.336E-02
 8.070E+01 2.798E-01 +-3.128E-02
 9.046E+01 3.006E-01 +-3.753E-02
 1.007E+02 3.027E-01 +-3.962E-02
 1.104E+02 3.152E-01 +-3.753E-02
 1.206E+02 3.215E-01 +-3.753E-02
 1.308E+02 3.486E-01 +-3.753E-02
 1.406E+02 3.528E-01 +-3.336E-02
 1.508E+02 3.486E-01 +-3.336E-02
 1.605E+02 3.382E-01 +-3.336E-02
 1.703E+02 3.277E-01 +-3.545E-02
 1.805E+02 2.902E-01 +-4.170E-02
 1.902E+02 2.485E-01 +-4.587E-02
 2.000E+02 1.818E-01 +-7.298E-02
 2.102E+02 1.422E-01 +-8.132E-02
 2.199E+02 1.067E-01 +-8.132E-02
 2.301E+02 1.109E-01 +-9.174E-02
 2.403E+02 5.250E-02 +-8.757E-02
 2.501E+02 3.374E-02 +-8.966E-02
 2.603E+02 2.957E-02 +-8.757E-02
 2.705E+02 1.914E-02 +-8.757E-02
 2.802E+02 1.497E-02 +-1.084E-01
 \END;
 /* Data scanned from Fig.1, p011601-2 in reference */

 \\EXP,3;
 /* 2006-09-14 : Altered, At. Re-digitized */
 RCT=12C(P,P)12C;

 \\DATA,3;
 THTL=50DEG;
 \DATA;
 ENGY-EMT-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
 (MEV) (MB/SR/MEV) (MB/SR/MEV)
 5.057E+01 2.837E-01 +-5.194E-02
 6.077E+01 2.816E-01 +-5.402E-02
 7.052E+01 2.816E-01 +-5.194E-02
 8.071E+01 2.858E-01 +-4.363E-02
 9.091E+01 2.837E-01 +-3.324E-02
 1.011E+02 2.983E-01 +-3.324E-02
 1.104E+02 3.024E-01 +-3.740E-02
 1.206E+02 3.170E-01 +-3.740E-02
 1.304E+02 2.796E-01 +-4.363E-02
 1.406E+02 2.484E-01 +-4.986E-02
 1.503E+02 2.152E-01 +-4.986E-02
 1.605E+02 1.466E-01 +-4.986E-02
 1.703E+02 1.341E-01 +-4.986E-02
 1.804E+02 1.050E-01 +-4.986E-02
 1.902E+02 7.387E-02 +-4.155E-02
 2.000E+02 4.271E-02 +-4.779E-02
 2.101E+02 4.894E-02 +-5.194E-02
 2.203E+02 2.401E-02 +-8.310E-02
 2.301E+02 2.609E-02 +-9.973E-02
 2.403E+02 1.362E-02 +-9.973E-02
 2.500E+02 1.155E-02 +-1.184E-01
 2.598E+02 1.570E-02 +-1.163E-01
 2.700E+02 1.155E-02 +-1.330E-01
 2.802E+02 1.362E-02 +-1.184E-01
 \END;
 /* Data scanned from Fig.1, p011601-2 in reference */
 \\END;