/*===================================================================*/
 /* NRDF D1751 Data No.23                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,23;
 D#=D1751;
 TITLE=/ Quasielastic pi- - nucleus scattering at 950 MeV/c /;
 ATH=(Y.FUJII'1', O.HASHIMOTO'1', T.NAKAWAGA'1', Y.SATO'1',
      T.TAKAHASHI'1', J.T.BRACK'2', C.J.GELDERLOOS'2', M.V.KEILMAN'2',
      R.J.PETERSON'2', M.ITOH'3', H.SAKAGUCHI'3', H.TAKEDA'3',
      K.AOKI'4', H.HOTCHI'4', H.NOUMI'4', Y.OHTA'4', H.OUTA'4',
      M.SEKIMOTO'4', M.YOUN'4', S.AJIMURA'5', T.KISHIMOTO'5',
      H.BHANG'6', H.PARK'6', R.SAWAFTA'7');
 INST-ATH=(2JPNTOH'1', 1USACLU'2', 2JPNKTO'3', 2JPNKEK'4', 2JPNOSA'5',
           3KORNSU'6', 1USAUSA'7');
      /* '1' Department of Physics */
      /* '2' Nuclear Physics Laboratory */
      /* '3' Department of Physics */
      /* '5' Department of Physics */
      /* '6' Department of Physics */
      /* '7' Physics Department, North Carolina A & T State University
 REF=PR/C;
 VLP=64(2001)034608;
 RCTS=(P(PIN,PIN)P, D(PIN,PIN)X, C(PIN,PIN)X, 208PB(PIN,PIN)X,
       6LI(PIN,PIN)X, CA(PIN,PIN)X, ZR(PIN,PIN)X);
 PHQS=(ANGL-DSTRN, ENGY-SPEC, ANGL-DSTRN'8', ENGY-SPEC'9', X'10');
 /* '8' integrated quasielastic cross section */
 /* '9' quasielastic cross section */
 /* '10' Quasielastic peak shifts relative to scattering from
    hydrogen */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,23;
 /* 2002-11-08 : Compiled, Nk + Im */
 /* 2004-10-13 : Converted, On. Converted from EXFOR E1751 */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN'11';
 /* '11' Negative-pion beam was delivered as a secondary beam
        from 12GeV proton synchrotron of the High Energy Accelerator
        Research Organization (KEK). */
 INST-ACC=2JPNKEK;
 ERS-PRJ=2.4%;
 BEAM-INTNSTY=XMA'12';
 /* '12' The typical beam intensity at the experimental target was
         1.1 x 10**6 particles/spill. wherethe beam duration was 1.8 s
         and the spill repetition cycle was 4 s. */
 POL-PRJ=0%;
 ION-SOURCE=/ Spallation /;
 DET-PARTCL=PIN;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'13',SCT'14');
 /* '13' Composite system with Drift Chamber+TOF+Aerogel
         Cerenkov+Lucite Cerenkov (Superconducting Kaon Spectrometer
         SKS [T.Fukuda et al., Nucl. Instrum. Methods Phys. Res.
         A361(1995)485]) */
 /* '14' Veto scintillator */
 SOLID-ANGL=100MSR;
 ERS-DET=3.0MEV'15';
 /* '15' for carbon elastic peak [FWHM] */
 /* 2006-10-13 : Altered, Mh. Re-digitized */
 RCT=C(PIN,PIN)X;
 RTY=X'93';
 /* '93' Quasielastic */
 PHQ=ENGY-SPEC'94';
 /* '94' quasielastic cross section */
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=4600MG/CM**2;
 INC-MOM-LAB=950MEV/C;
 ANL=RPA'95';
 /* '95' Finite-nucleus continuum RPA framework using
         density-dependent particle-hole interaction [A.De Pace
         (private communication)] */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,23;
 SYS-ERR=11%'16';
 /* '16' Back ground subtraction */
 INC-MOM-LAB=950MEV/C;
 TRNSF-MOM=550MEV/C'96';
 /* '96' Transferred momentum q=550MeV/c */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 TRNSF-ENGY DSIGMA/DOMEGA/DE
 (MEV) (MB/SR/MEV)
 -3.300E+01 1.270E-04
 -2.810E+01 2.726E-05
 -2.273E+01 2.726E-05
 -1.783E+01 -7.243E-05
 -1.293E+01 -7.243E-05
 -8.023E+00 -7.243E-05
 -2.421E+00 -7.243E-05
 2.248E+00 -1.721E-04
 7.150E+00 1.270E-04
 1.252E+01 2.726E-05
 1.742E+01 1.423E-03
 2.232E+01 4.713E-03
 2.769E+01 8.999E-03
 3.259E+01 7.803E-03
 3.726E+01 9.299E-03
 4.216E+01 1.040E-02
 4.777E+01 1.030E-02
 5.267E+01 1.119E-02
 5.687E+01 1.319E-02
 6.294E+01 1.339E-02
 6.714E+01 1.568E-02
 7.228E+01 1.478E-02
 7.788E+01 1.757E-02
 8.231E+01 2.086E-02
 8.722E+01 2.395E-02
 9.212E+01 2.784E-02
 9.772E+01 2.964E-02
 1.022E+02 3.283E-02
 1.073E+02 3.831E-02
 1.129E+02 3.941E-02
 1.171E+02 4.240E-02
 1.222E+02 4.309E-02
 1.274E+02 4.469E-02
 1.323E+02 4.728E-02
 1.369E+02 4.937E-02
 1.425E+02 4.987E-02
 1.474E+02 5.147E-02
 1.521E+02 5.147E-02
 1.572E+02 5.256E-02
 1.621E+02 5.575E-02
 1.670E+02 5.605E-02
 1.729E+02 5.595E-02
 1.778E+02 5.546E-02
 1.825E+02 5.147E-02
 1.874E+02 5.177E-02
 1.925E+02 4.967E-02
 1.976E+02 4.708E-02
 2.028E+02 4.279E-02
 2.072E+02 3.950E-02
 2.126E+02 3.602E-02
 2.170E+02 3.173E-02
 2.221E+02 2.993E-02
 2.277E+02 2.694E-02
 2.324E+02 2.316E-02
 2.371E+02 2.007E-02
 2.429E+02 1.967E-02
 2.476E+02 1.618E-02
 2.525E+02 1.239E-02
 2.574E+02 1.049E-02
 2.628E+02 8.999E-03
 2.677E+02 8.501E-03
 2.721E+02 5.809E-03
 2.777E+02 3.417E-03
 2.826E+02 3.915E-03
 2.873E+02 2.420E-03
 2.929E+02 1.024E-03
 3.020E+02 1.024E-03
 3.076E+02 1.323E-03
 3.176E+02 1.270E-04
 3.223E+02 3.417E-03
 3.277E+02 8.248E-04
 3.326E+02 4.260E-04
 3.375E+02 4.214E-03
 3.431E+02 7.251E-04
 3.473E+02 2.420E-03
 3.526E+02 3.915E-03
 \END;
 /*===================================================================*/