/*===================================================================*/
 /* NRDF D1751 Data No.22                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,22;
 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,22;
 /* 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'89';
 /* '89' Quasielastic */
 PHQ=ENGY-SPEC'90';
 /* '90' quasielastic cross section */
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=4600MG/CM**2;
 INC-MOM-LAB=950MEV/C;
 ANL=RPA'91';
 /* '91' Finite-nucleus continuum RPA framework using
         density-dependent particle-hole interaction [A.De Pace
         (private communication)] */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,22;
 SYS-ERR=11%'16';
 /* '16' Back ground subtraction */
 INC-MOM-LAB=950MEV/C;
 TRNSF-MOM=450MEV/C'92';
 /* '92' Transferred momentum q=450MeV/c */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 TRNSF-ENGY DSIGMA/DOMEGA/DE
 (MEV) (MB/SR/MEV)
 -3.318E+01 1.721E-04
 -2.813E+01 1.721E-04
 -2.285E+01 8.903E-04
 -1.781E+01 1.721E-04
 -1.300E+01 1.721E-04
 -8.197E+00 8.903E-04
 -2.433E+00 8.903E-04
 6.937E+00 1.382E-02
 1.222E+01 5.439E-03
 1.727E+01 2.555E-02
 2.183E+01 1.837E-02
 2.760E+01 2.363E-02
 3.216E+01 2.962E-02
 3.697E+01 3.512E-02
 4.201E+01 4.350E-02
 4.706E+01 4.829E-02
 5.210E+01 5.930E-02
 5.715E+01 6.313E-02
 6.243E+01 7.271E-02
 6.724E+01 8.564E-02
 7.229E+01 9.425E-02
 7.757E+01 1.014E-01
 8.238E+01 1.069E-01
 8.694E+01 1.163E-01
 9.175E+01 1.203E-01
 9.727E+01 1.235E-01
 1.023E+02 1.306E-01
 1.071E+02 1.282E-01
 1.126E+02 1.302E-01
 1.174E+02 1.242E-01
 1.222E+02 1.196E-01
 1.275E+02 1.215E-01
 1.323E+02 1.151E-01
 1.374E+02 1.113E-01
 1.427E+02 1.084E-01
 1.477E+02 1.019E-01
 1.525E+02 9.138E-02
 1.573E+02 8.133E-02
 1.624E+02 7.415E-02
 1.674E+02 6.529E-02
 1.722E+02 5.930E-02
 1.777E+02 4.805E-02
 1.825E+02 4.350E-02
 1.873E+02 3.273E-02
 1.926E+02 2.962E-02
 1.974E+02 2.555E-02
 2.024E+02 1.884E-02
 2.075E+02 1.741E-02
 2.128E+02 1.430E-02
 2.173E+02 1.047E-02
 2.226E+02 7.354E-03
 2.277E+02 6.396E-03
 2.325E+02 4.481E-03
 2.373E+02 4.242E-03
 2.430E+02 2.087E-03
 2.476E+02 1.721E-04
 2.522E+02 -6.732E-05
 2.572E+02 8.903E-04
 2.625E+02 -3.067E-04
 2.673E+02 1.848E-03
 2.723E+02 3.763E-03
 2.776E+02 4.242E-03
 2.827E+02 3.524E-03
 2.875E+02 5.199E-03
 2.925E+02 3.045E-03
 2.978E+02 5.199E-03
 3.026E+02 9.748E-03
 3.074E+02 8.551E-03
 3.127E+02 9.509E-03
 3.180E+02 1.094E-02
 3.223E+02 8.072E-03
 3.278E+02 1.214E-02
 3.331E+02 1.406E-02
 \END;
 /*===================================================================*/