/*===================================================================*/
 /* NRDF D1751 Data No.26                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,26;
 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,26;
 /* 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=6LI(PIN,PIN)X;
 RTY=X'107';
 /* '107' Quasielastic */
 PHQ=X'108';
 /* '108' Quasielastic peak shifts relative to scattering from
          hydrogen */
 ENR=X%'109';
 /* '109' Hihgly isotopically enriched CD2 and 6LiD2, and natural
          isotopic C */
 CHM=X'110';
 /* '110' CD2 and C */
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2'111';
 /* '111' 1.4g/cm2 for CD2, 2.0g/cm2 for 6LiD2, and 4.6g/cm2 for
          C */
 INC-MOM-LAB=950MEV/C;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,26;
 SYS-ERR=11%'16';
 /* '16' Back ground subtraction */
 INC-MOM-LAB=950MEV/C;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 TRNSF-MOM DATA1'112' DELTA-DATA1'112'
 (MEV/C) (MEV) (MEV)
 3.506E+02 -4.415E+00 +-NEGLIGIBLE
 3.768E+02 -3.911E+00 +-NEGLIGIBLE
 4.012E+02 -2.651E+00 +-NEGLIGIBLE
 4.256E+02 -1.309E-01 +-NEGLIGIBLE
 4.517E+02 1.507E+00 +-NEGLIGIBLE
 4.756E+02 -1.309E-01 +-NEGLIGIBLE
 5.000E+02 3.271E+00 +-NEGLIGIBLE
 5.262E+02 7.302E+00 +-NEGLIGIBLE
 5.500E+02 8.184E+00 +-NEGLIGIBLE
 5.756E+02 1.524E+01 +-2.898E+00
 6.000E+02 1.436E+01 +-3.024E+00
 \END;
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