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| /*===================================================================*/
/* NRDF D1731 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
D#=D1731;
TITLE=/ Asymmetry in the nonmesonic weak decay of polarized
5(Lambda)He hypernuclei /;
PURPOSE=/ To present a measurement of the asymmetrion emission from
thenon mesonic decay, and derive the asymmetry parameter of
the non mesonic decay using the measured polarization /;
ATH=(S.AJIMURA'1', K.IKEDA'1', M.ISHIKAWA'1', T.KISHIMOTO'1',
A.OKUSU'1', N.SHINKAI'1', Y.TANAKA'1', H.EJIRI'2', T.NAKANO'2',
K.MANABE'3', T.NAGAE'3', H.NOUMI'3', M.SEKIMOTO'3', T.SHIBATA'3',
O.HASHIMOTO'4', K.MAEDA'4', T.TAKAHASHI'4', T.HASEGAWA'5',
H.BHANG'6', Y.D.KIM'6', H.PARK'6', M.YOUN'6');
INST-ATH=(2JPNOSA'1', 2JPNRCN'2', 2JPNKEK'3', 2JPNTOH'4', 2JPNJPN'5',
3KORNSU'6');
/* '1' Department of Physics */
/* '4' Department of Physics */
/* '5' School of Hygienic Science, Kitazato University,
Sagamihara, Kangawa */
/* '6' Department of Physics */
REF=PRL;
VLP=84(2000)4052;
RCTS=6LI(PIP,KP)X;
PHQS=;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,1;
/* 2002-10-02 : Converted, Data cannot converted to EXFOR E1731 */
ENR=95%'7';
/* '7' value found in S.Ajimura et al.,PRL80(1998)3471 */
CHM=ELM;
PHYS-FORM=SLD;
BAC=X;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=SYN;
INST-ACC=2JPNKEK'8';
/* '8' K6 beam line of KEK-PS */
INC-MOM-LAB=1.05GEV/C;
BEAM-INTNSTY=XNA'9';
/* '9' about 3e06/spill, where a spill consisted of 1.7 secof
continuous beam every 4.0sec [S.Ajimura et
al.,PRL80(1998)3471]) */
CHRG-INC-ION=1;
POL-PRJ=0%;
ANT-COINC=NO;
DET-SYS=MAG'10';
/* '10' SKS (Superconducting Kaon Spectrometer), see [T.Fukuda et
al.,Nucl.Instrum.Methods Phys.Res.Sect.A361(1995)485] */
SOLID-ANGL=[100MSR'11';
/* '11' found in [S.Ajimura et al.,PRL80(1998)3471] */
ERS-DET=2MEV'12';
/* '12' FWHM, found in [S.Ajimura et al.,PRL80(1998)3471] */
/* 2006-08-22 : Altered, At. Re-digitized */
RCT=6LI(PIP,KP)X;
DET-PARTCL=KP;
COINC=NO;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
INC-MOM-LAB=1.05GEV/C;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY'13' COUNTS'14' DELTA-COUNTS'14'
(MEV) (ARB) (ARB)
-8.750E+00 3.125E+01 +-1.042E+01
-8.250E+00 3.125E+01 +-1.042E+01
-7.750E+00 4.167E+01 +-1.042E+01
-7.250E+00 6.250E+01 +-1.042E+01
-6.750E+00 5.208E+01 +-1.042E+01
-6.250E+00 6.250E+01 +-1.042E+01
-5.750E+00 7.292E+01 +-1.042E+01
-5.312E+00 8.333E+01 +-1.042E+01
-4.812E+00 9.375E+01 +-1.042E+01
-4.250E+00 1.354E+02 +-1.042E+01
-3.760E+00 1.462E+02 +-1.077E+01
-3.250E+00 1.875E+02 +-1.042E+01
-2.750E+00 2.604E+02 +-2.083E+01
-2.250E+00 3.542E+02 +-2.083E+01
-1.750E+00 5.208E+02 +-2.083E+01
-1.250E+00 7.500E+02 +-3.125E+01
-7.500E-01 9.792E+02 +-3.125E+01
-2.506E-01 1.135E+03 +-3.482E+01
2.506E-01 1.197E+03 +-4.280E+01
7.520E-01 1.156E+03 +-4.178E+01
1.253E+00 1.044E+03 +-3.955E+01
1.671E+00 9.679E+02 +-3.481E+01
2.250E+00 9.271E+02 +-3.125E+01
2.750E+00 7.708E+02 +-3.125E+01
3.175E+00 6.824E+02 +-2.786E+01
3.676E+00 6.754E+02 +-3.482E+01
4.178E+00 6.407E+02 +-2.786E+01
4.679E+00 6.197E+02 +-3.482E+01
5.264E+00 7.172E+02 +-3.482E+01
5.682E+00 6.893E+02 +-3.482E+01
6.183E+00 7.172E+02 +-3.482E+01
6.685E+00 7.382E+02 +-2.785E+01
7.186E+00 8.425E+02 +-3.001E+01
7.750E+00 9.271E+02 +-3.125E+01
8.250E+00 9.063E+02 +-3.125E+01
8.690E+00 1.003E+03 +-3.403E+01
9.250E+00 1.104E+03 +-4.167E+01
9.777E+00 1.163E+03 +-3.481E+01
1.025E+01 1.219E+03 +-3.125E+01
1.075E+01 1.344E+03 +-4.167E+01
1.125E+01 1.312E+03 +-4.167E+01
1.169E+01 1.441E+03 +-3.449E+01
1.225E+01 1.458E+03 +-3.125E+01
1.275E+01 1.490E+03 +-4.167E+01
1.325E+01 1.542E+03 +-4.167E+01
1.375E+01 1.562E+03 +-4.167E+01
1.425E+01 1.667E+03 +-4.167E+01
1.475E+01 1.625E+03 +-4.167E+01
1.525E+01 1.719E+03 +-4.167E+01
1.575E+01 1.792E+03 +-4.167E+01
1.625E+01 1.990E+03 +-5.208E+01
1.675E+01 2.156E+03 +-5.208E+01
1.725E+01 2.354E+03 +-5.208E+01
1.775E+01 2.479E+03 +-5.208E+01
1.825E+01 2.542E+03 +-5.208E+01
1.875E+01 2.719E+03 +-5.208E+01
1.925E+01 2.823E+03 +-5.208E+01
1.972E+01 2.911E+03 +-5.815E+01
2.022E+01 3.022E+03 +-5.570E+01
2.072E+01 3.329E+03 +-5.682E+01
2.122E+01 3.384E+03 +-5.570E+01
2.175E+01 3.469E+03 +-6.250E+01
2.225E+01 3.469E+03 +-6.250E+01
2.272E+01 3.558E+03 +-6.265E+01
2.325E+01 3.667E+03 +-6.250E+01
2.373E+01 3.732E+03 +-6.007E+01
2.423E+01 3.635E+03 +-6.332E+01
2.475E+01 3.688E+03 +-6.250E+01
2.525E+01 3.802E+03 +-6.250E+01
2.575E+01 3.760E+03 +-6.250E+01
2.625E+01 3.885E+03 +-6.250E+01
2.675E+01 3.896E+03 +-6.250E+01
2.725E+01 3.833E+03 +-6.250E+01
2.775E+01 3.896E+03 +-6.250E+01
2.824E+01 3.914E+03 +-6.960E+01
2.874E+01 3.934E+03 +-6.265E+01
2.925E+01 3.896E+03 +-6.250E+01
2.974E+01 3.927E+03 +-5.160E+01
\END;
/*===================================================================*/
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