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| /*===================================================================*/
/* NRDF D1609 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
D#=D1609;
TITLE=/ Two-nucleon pion absorption in 4He at 1 GeV/c /;
PURPOSE=/ The first measurment of two-nucleon pion absorption in 4he
at1gev/c /;
ATH=(T.NAGAE'1', T.FUKUDA'1', M.SEKIMOTO'1', T.MIYACHI'1',
P.KITCHING'1', I.NOMURA'2', I.ARAI'3', K.TOMIZAWA'3',
H.KITAYAMA'3', Y.NAGASAKA'3', S.UENO'3', K.WAKI'3', K.MAEDA'4',
T.SUDA'4', H.MATSUYAMA'5', T.KOBAYASHI'6', D.ROWNTREE'7',
M.A.PROHVATILOV'8', V.I.RASIN'8');
INST-ATH=(2JPNINS'1', 2JPNIPC'2', 2JPNTSU'3', 2JPNTOH'4', 2JPNTOH'5',
2JPNKEK'6', 1USAMIT'7', 4RUSJIA'8');
/* '3' Institute of Physics */
/* '4' College of General Education */
/* '5' Laboratory of Nuclear Science */
REF=PL/B;
VLP=335(1994)330;
RCTS=(4HE(PIP,P,P)X, 4HE(PIP,N,P)X);
PHQS=ANGL-DSTRN;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,1;
/* 2003-10-02 : Converted, Nk + Am + On. Converted to EXFOR E1609
/* 2005-11-03 : Converted, On. Converted from EXFOR E1609 */
/* Related references
- none, E1838001, J(Phys)149.
PHQ=ANGL-DSTRN;
CHM=ELM;
PHYS-FORM=LIQD;
THK-TGT=2800MG/CM**2;
BAC=X'9';
/* '9' cylindrical container made of stainless steel */
THK-BAC=XMG/CM**2'10';
/* '10' a window thickness of 0.5 mm */
POL-TGT=0%;
ALGN-TGT=0%;
ACC=SYN'11';
/* '11' KEK 12GeV proton synchrotron */
INST-ACC=2JPNKEK;
INC-MOM-LAB=1GEV/C;
ERS-PRJ=1.5%;
BEAM-INTNSTY=XPNA'12';
/* '12' 10**5 particles/spill */
POL-PRJ=0%;
ION-SOURCE=/ Spallation /;
ANT-COINC=NO;
DET-SYS=(MAG'13',SCT'14',SCT'15',TOF);
/* '13' Dipole magnet to analyze the momentum of the
forward-scattered charged particles. Efficiency of the
spectrometer was estimated to be 59+-3 % for high-momentum
protons. */
/* '14' Nine plastic scintillators to identify forward-scattered
charged particles (ToF wall). */
/* '15' Two ToF walls (NHA and HNB) to detect protons and
neutrons. Detection efficiencies for neutron is 11+-1 % for
400 MeV/c to 950 MeV/c neutron, while 10+-1 % for neutrons
with same momentum range. */
/* 2006-12-19 : Altered, At. Re-digitized */
RCT=4HE(PIP,P,P)X;
RTY=X'16';
/* '16' pion absorption */
DET-PARTCL=P;
COINC=(P,P);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
INC-MOM-LAB=1GEV/C;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTL DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA'17'
(DEG) (UB/SR) (UB/SR)
4.555E+00 5.512E+02 +-NEGLIGIBLE
7.531E+00 4.756E+02 +-NEGLIGIBLE
1.052E+01 1.936E+02 +-NEGLIGIBLE
1.350E+01 1.740E+02 +-NEGLIGIBLE
1.653E+01 1.894E+02 +-3.069E+01
1.951E+01 1.368E+02 +-NEGLIGIBLE
2.249E+01 9.108E+01 +-NEGLIGIBLE
2.547E+01 6.856E+01 +-1.115E+01
2.856E+01 8.671E+01 +-NEGLIGIBLE
3.153E+01 9.831E+01 +-NEGLIGIBLE
3.451E+01 6.817E+01 +-NEGLIGIBLE
\END;
/*===================================================================*/
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