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| /*===================================================================*/
/* NRDF D1751 Data No.11 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,11;
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,11;
/* 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'56';
/* '56' Quasielastic */
PHQ=ENGY-SPEC;
ENR=NAT;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=4600MG/CM**2;
INC-MOM-LAB=950MEV/C;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,11;
SYS-ERR=11%'16';
/* '16' Back ground subtraction */
INC-MOM-LAB=950MEV/C;
TRNSF-MOM=650MEV/C'57';
/* '57' Momentum transfer q=650MeV/c */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
TRNSF-ENGY DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
(MEV) (MB/SR/MEV) (MB/SR/MEV)
-3.315E+01 -6.702E-04 +-NEGLIGIBLE
-2.495E+01 -6.702E-04 +-NEGLIGIBLE
-1.635E+01 -6.702E-04 +-NEGLIGIBLE
-8.540E+00 -6.702E-04 +-NEGLIGIBLE
-7.256E-01 -1.050E-03 +-NEGLIGIBLE
6.307E+00 -6.702E-04 +-NEGLIGIBLE
1.451E+01 -1.050E-03 +-NEGLIGIBLE
1.842E+01 6.540E-03 +-NEGLIGIBLE
2.428E+01 1.072E-02 +-NEGLIGIBLE
2.897E+01 6.161E-03 +-NEGLIGIBLE
3.394E+01 2.626E-02 +-NEGLIGIBLE
3.847E+01 2.130E-02 +-NEGLIGIBLE
4.442E+01 3.369E-02 +-NEGLIGIBLE
4.924E+01 3.948E-02 +-NEGLIGIBLE
5.462E+01 5.352E-02 +-NEGLIGIBLE
5.916E+01 5.683E-02 +-NEGLIGIBLE
6.398E+01 5.903E-02 +-NEGLIGIBLE
6.851E+01 6.839E-02 +-NEGLIGIBLE
7.389E+01 7.307E-02 +-NEGLIGIBLE
7.928E+01 7.913E-02 +-NEGLIGIBLE
8.494E+01 8.547E-02 +-NEGLIGIBLE
8.835E+01 9.097E-02 +-NEGLIGIBLE
9.430E+01 1.050E-01 +-5.508E-03
9.855E+01 1.144E-01 +-5.783E-03
1.036E+02 1.243E-01 +-6.609E-03
1.107E+02 1.246E-01 +-NEGLIGIBLE
1.138E+02 1.337E-01 +-NEGLIGIBLE
1.189E+02 1.524E-01 +-7.160E-03
1.240E+02 1.529E-01 +-6.609E-03
1.294E+02 1.628E-01 +-NEGLIGIBLE
1.343E+02 1.835E-01 +-8.812E-03
1.388E+02 1.769E-01 +-7.160E-03
1.433E+02 1.898E-01 +-8.261E-03
1.490E+02 2.132E-01 +-7.986E-03
1.547E+02 2.256E-01 +-8.537E-03
1.592E+02 2.479E-01 +-8.261E-03
1.640E+02 2.702E-01 +-9.914E-03
1.691E+02 2.590E-01 +-1.046E-02
1.742E+02 2.873E-01 +-1.129E-02
1.790E+02 3.047E-01 +-9.363E-03
1.836E+02 2.917E-01 +-1.046E-02
1.898E+02 2.997E-01 +-1.184E-02
1.938E+02 3.267E-01 +-1.239E-02
1.986E+02 3.361E-01 +-1.102E-02
2.031E+02 3.286E-01 +-1.046E-02
2.091E+02 3.344E-01 +-1.129E-02
2.150E+02 3.383E-01 +-1.239E-02
2.187E+02 3.586E-01 +-1.074E-02
2.232E+02 3.369E-01 +-1.102E-02
2.286E+02 3.529E-01 +-1.102E-02
2.346E+02 3.606E-01 +-1.239E-02
2.388E+02 3.405E-01 +-1.046E-02
2.436E+02 3.752E-01 +-1.239E-02
2.484E+02 3.653E-01 +-1.294E-02
2.538E+02 3.286E-01 +-1.322E-02
2.592E+02 3.187E-01 +-1.377E-02
2.637E+02 3.273E-01 +-1.294E-02
2.691E+02 3.286E-01 +-1.294E-02
2.745E+02 3.358E-01 +-1.267E-02
2.793E+02 3.146E-01 +-1.239E-02
2.836E+02 3.088E-01 +-1.322E-02
2.890E+02 3.160E-01 +-1.377E-02
2.946E+02 2.950E-01 +-1.377E-02
2.986E+02 2.669E-01 +-1.294E-02
3.031E+02 2.427E-01 +-1.349E-02
3.085E+02 2.292E-01 +-1.432E-02
3.150E+02 2.493E-01 +-1.625E-02
3.199E+02 2.389E-01 +-1.625E-02
3.227E+02 2.281E-01 +-1.515E-02
3.284E+02 2.141E-01 +-1.570E-02
3.343E+02 1.923E-01 +-1.432E-02
3.386E+02 2.441E-01 +-1.762E-02
3.434E+02 2.237E-01 +-1.707E-02
3.485E+02 2.342E-01 +-1.680E-02
3.539E+02 2.204E-01 +-1.625E-02
3.590E+02 1.995E-01 +-1.625E-02
\END;
/*===================================================================*/
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