/*===================================================================*/
 /* NRDF D1751 Data No.21                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,21;
 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,21;
 /* 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'85';
 /* '85' Quasielastic */
 PHQ=ENGY-SPEC'86';
 /* '86' quasielastic cross section */
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=4600MG/CM**2;
 INC-MOM-LAB=950MEV/C;
 ANL=RPA'87';
 /* '87' Finite-nucleus continuum RPA framework using
         density-dependent particle-hole interaction [A.De Pace
         (private communication)] */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,21;
 SYS-ERR=11%'16';
 /* '16' Back ground subtraction */
 INC-MOM-LAB=950MEV/C;
 TRNSF-MOM=350MEV/C'88';
 /* '88' Transferred momentum q=350MeV/c */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 TRNSF-ENGY DSIGMA/DOMEGA/DE
 (MEV) (MB/SR/MEV)
 -9.073E+00 1.264E-04
 6.112E+00 2.647E-02
 1.166E+01 1.722E-01
 1.648E+01 2.916E-01
 2.130E+01 1.565E-01
 2.660E+01 1.672E-01
 3.142E+01 2.030E-01
 3.648E+01 2.395E-01
 4.106E+01 2.596E-01
 4.637E+01 2.776E-01
 5.143E+01 2.804E-01
 5.649E+01 2.916E-01
 6.179E+01 2.994E-01
 6.613E+01 3.073E-01
 7.167E+01 3.073E-01
 7.674E+01 2.882E-01
 8.156E+01 2.893E-01
 8.638E+01 2.675E-01
 9.144E+01 2.473E-01
 9.674E+01 2.238E-01
 1.016E+02 2.013E-01
 1.061E+02 1.722E-01
 1.119E+02 1.470E-01
 1.165E+02 1.313E-01
 1.213E+02 1.049E-01
 1.269E+02 8.869E-02
 1.317E+02 7.131E-02
 1.365E+02 6.122E-02
 1.418E+02 4.889E-02
 1.469E+02 4.104E-02
 1.517E+02 3.488E-02
 1.565E+02 2.759E-02
 1.618E+02 2.143E-02
 1.666E+02 1.358E-02
 1.717E+02 7.413E-03
 1.770E+02 4.610E-03
 1.816E+02 2.368E-03
 1.866E+02 2.368E-03
 1.920E+02 -4.342E-04
 1.968E+02 1.808E-03
 2.168E+02 2.368E-03
 2.218E+02 6.852E-03
 2.269E+02 1.808E-03
 2.320E+02 4.050E-03
 2.365E+02 1.806E-02
 2.423E+02 2.087E-02
 \END;
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