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| /*===================================================================*/
/* NRDF D1751 Data No.15 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,15;
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,15;
/* 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=D(PIN,PIN)X;
RTY=X'66';
/* '66' Quasielastic */
PHQ=ANGL-DSTRN'67';
/* '67' integrated quasielastic cross section */
ENR=X%'68';
/* '68' Hihgly isotopically enriched CD2 and natural isotopic C
CHM=X'69';
/* '69' CD2 and C */
PHYS-FORM=SLD;
THK-TGT=XMG/CM**2'70';
/* '70' 1.4g/cm2 for CD2 and 4.6g/cm2 for C */
INC-MOM-LAB=950MEV/C;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,15;
SYS-ERR=11%'16';
/* '16' Back ground subtraction */
INC-MOM-LAB=950MEV/C;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
TRNSF-MOM DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(MEV/C) (MB/SR) (MB/SR)
3.512E+02 1.377E+01 +1.533E+00-1.524E+00
3.749E+02 1.173E+01 +1.357E+00-1.420E+00
4.013E+02 9.919E+00 +1.278E+00-1.234E+00
4.245E+02 8.450E+00 +1.088E+00-1.052E+00
4.505E+02 7.486E+00 +9.643E-01-9.826E-01
4.749E+02 6.402E+00 +7.965E-01-8.404E-01
5.010E+02 5.454E+00 +7.026E-01-7.344E-01
5.251E+02 4.738E+00 +7.159E-01-5.243E-01
5.498E+02 3.852E+00 +4.623E-01-5.316E-01
5.753E+02 3.320E+00 +4.571E-01-4.245E-01
6.003E+02 2.678E+00 +4.532E-01-3.515E-01
6.264E+02 2.264E+00 +3.727E-01-3.048E-01
6.505E+02 2.077E+00 +3.326E-01-2.797E-01
\END;
/*===================================================================*/
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