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| /*===================================================================*/
/* NRDF D1751 Data No.10 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,10;
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,10;
/* 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'54';
/* '54' Quasielastic */
PHQ=ENGY-SPEC;
ENR=NAT;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=4600MG/CM**2;
INC-MOM-LAB=950MEV/C;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,10;
SYS-ERR=11%'16';
/* '16' Back ground subtraction */
INC-MOM-LAB=950MEV/C;
TRNSF-MOM=500MEV/C'55';
/* '55' Momentum transfer q=500MeV/c */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
TRNSF-ENGY DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
(MEV) (MB/SR/MEV) (MB/SR/MEV)
-3.331E+01 -3.033E-04 +-NEGLIGIBLE
-2.601E+01 -3.033E-04 +-NEGLIGIBLE
-1.871E+01 -3.033E-04 +-NEGLIGIBLE
-1.141E+01 -3.033E-04 +-NEGLIGIBLE
-3.473E+00 -3.033E-04 +-NEGLIGIBLE
4.145E+00 -2.210E-04 +-NEGLIGIBLE
8.907E+00 3.975E-03 +-NEGLIGIBLE
1.430E+01 1.928E-02 +-NEGLIGIBLE
1.875E+01 2.709E-02 +-NEGLIGIBLE
2.478E+01 1.319E-02 +-NEGLIGIBLE
2.954E+01 1.080E-02 +-NEGLIGIBLE
3.398E+01 1.475E-02 +-NEGLIGIBLE
3.906E+01 1.796E-02 +-NEGLIGIBLE
4.446E+01 2.035E-02 +-NEGLIGIBLE
4.922E+01 2.249E-02 +-NEGLIGIBLE
5.462E+01 2.495E-02 +-NEGLIGIBLE
5.843E+01 3.022E-02 +-NEGLIGIBLE
6.382E+01 3.507E-02 +-NEGLIGIBLE
6.890E+01 4.190E-02 +-NEGLIGIBLE
7.430E+01 4.749E-02 +-NEGLIGIBLE
7.906E+01 5.334E-02 +-NEGLIGIBLE
8.414E+01 5.844E-02 +-NEGLIGIBLE
8.890E+01 6.617E-02 +-NEGLIGIBLE
9.430E+01 6.921E-02 +-NEGLIGIBLE
9.937E+01 7.703E-02 +-1.563E-03
1.045E+02 8.016E-02 +-NEGLIGIBLE
1.092E+02 8.468E-02 +-NEGLIGIBLE
1.133E+02 8.945E-02 +-NEGLIGIBLE
1.187E+02 9.036E-02 +-NEGLIGIBLE
1.245E+02 9.258E-02 +-NEGLIGIBLE
1.292E+02 9.760E-02 +-NEGLIGIBLE
1.346E+02 9.653E-02 +-NEGLIGIBLE
1.432E+02 9.472E-02 +-NEGLIGIBLE
1.492E+02 9.982E-02 +-1.974E-03
1.546E+02 9.324E-02 +-1.563E-03
1.597E+02 9.702E-02 +-1.892E-03
1.648E+02 9.241E-02 +-1.563E-03
1.692E+02 8.838E-02 +-NEGLIGIBLE
1.740E+02 8.921E-02 +-1.645E-03
1.794E+02 8.139E-02 +-1.810E-03
1.832E+02 7.777E-02 +-1.563E-03
1.895E+02 7.201E-02 +-NEGLIGIBLE
1.937E+02 6.601E-02 +-NEGLIGIBLE
1.987E+02 6.132E-02 +-NEGLIGIBLE
2.041E+02 5.482E-02 +-NEGLIGIBLE
2.092E+02 5.046E-02 +-NEGLIGIBLE
2.143E+02 4.856E-02 +-NEGLIGIBLE
2.187E+02 4.379E-02 +-NEGLIGIBLE
2.244E+02 4.281E-02 +-NEGLIGIBLE
2.292E+02 4.067E-02 +-NEGLIGIBLE
2.343E+02 3.812E-02 +-NEGLIGIBLE
2.390E+02 3.524E-02 +-NEGLIGIBLE
2.441E+02 3.318E-02 +-NEGLIGIBLE
2.489E+02 3.260E-02 +-NEGLIGIBLE
2.536E+02 3.055E-02 +-NEGLIGIBLE
2.590E+02 3.063E-02 +-NEGLIGIBLE
2.641E+02 2.923E-02 +-NEGLIGIBLE
2.692E+02 2.660E-02 +-NEGLIGIBLE
2.743E+02 2.874E-02 +-NEGLIGIBLE
2.784E+02 3.088E-02 +-NEGLIGIBLE
2.838E+02 2.767E-02 +-NEGLIGIBLE
2.886E+02 3.219E-02 +-1.399E-03
2.946E+02 3.022E-02 +-NEGLIGIBLE
2.978E+02 3.252E-02 +-NEGLIGIBLE
3.035E+02 3.499E-02 +-NEGLIGIBLE
3.092E+02 3.581E-02 +-2.057E-03
3.143E+02 3.367E-02 +-1.728E-03
3.197E+02 3.384E-02 +-1.892E-03
3.232E+02 3.738E-02 +-NEGLIGIBLE
3.279E+02 3.853E-02 +-1.728E-03
3.343E+02 3.836E-02 +-1.563E-03
\END;
/*===================================================================*/
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