/*===================================================================*/
 /* NRDF D1751 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 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,2;
 /* 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=P(PIN,PIN)P;
 RTY=(ELA-SCATT,X'21');
 /* '21' Quasielastic */
 PHQ=ANGL-DSTRN;
 ENR=NAT;
 CHM=X'22';
 /* '22' CH2 and C */
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2'23';
 /* '23' 3.5g/cm2 for CH2 and 4.6g/cm2 for C */
 INC-MOM-LAB=1050MEV/C;
 ANL=PSHIFT-ANL'24';
 /* '24' SAID [R.A.Arndt, I.I.Strakovsky, R.L.Workman, and
         M.M.Pavan, Phys.Rev.C52(1995)2120] */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 SYS-ERR=11%'16';
 /* '16' Back ground subtraction */
 INC-MOM-LAB=1050MEV/C;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTL DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (MB/SR) (MB/SR)
 2.251E+01 1.141E+01 +-NEGLIGIBLE
 2.357E+01 1.037E+01 +-NEGLIGIBLE
 2.451E+01 8.302E+00 +-NEGLIGIBLE
 2.551E+01 7.119E+00 +-NEGLIGIBLE
 2.649E+01 5.758E+00 +-NEGLIGIBLE
 2.752E+01 4.707E+00 +-NEGLIGIBLE
 2.855E+01 3.828E+00 +-NEGLIGIBLE
 2.949E+01 3.113E+00 +-NEGLIGIBLE
 3.052E+01 2.491E+00 +-NEGLIGIBLE
 3.153E+01 1.861E+00 +-NEGLIGIBLE
 3.250E+01 1.383E+00 +-NEGLIGIBLE
 3.353E+01 9.050E-01 +-NEGLIGIBLE
 3.450E+01 7.398E-01 +-NEGLIGIBLE
 3.556E+01 5.104E-01 +-NEGLIGIBLE
 3.654E+01 3.184E-01 +-NEGLIGIBLE
 3.754E+01 2.469E-01 +-2.718E-02
 3.857E+01 1.363E-01 +-2.098E-02
 3.960E+01 1.150E-01 +-2.200E-02
 4.054E+01 9.918E-02 +-2.022E-02
 4.155E+01 1.445E-01 +-2.402E-02
 4.255E+01 9.761E-02 +-2.053E-02
 4.352E+01 1.422E-01 +-2.364E-02
 \END;
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