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/* NRDF D1800 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
D#=D1800;
TITLE=/Gamow-Teller transitions from 58Ni to discrete states of 58Cu/;
PURPOSE=/To investigate the Tz=1 -> 0 transitions to GT states in 58Cu.
ATH=(Y.FUJITA'1', H.FUJITA'1', T.ADACHI'1', G.P.A.BERG'2',
E.CAURIER'3', H.FUJIMURA'2', K.HARA'2', K.HATANAKA'2',
Z.JANAS'4,5', J.KAMIYA'2', T.KAWABATA'6', K.LANGANKE'7',
G.MARTINEZ-PINEDO'7', T.NORO'2', E.ROECKL'4', Y.SHIMBARA'1',
T.SHINADA'1', S.Y.VAN DER WERF'8', M.YOSHIFUKU'1', M.YOSOI'6',
R.G.T.ZEGERS'9');
INST-ATH=(2JPNOSA'1', 2JPNOSA'2', 2FR FR'3', 2GERGSI'4', 3POLWWA'5',
2JPNKTO'6', 2DENAAU'7', 2NEDGRN'8', 2JPNJAE'9');
/* '1' Department of Physics */
/* '2' Research Cneter for Nuclear Physics */
/* '3' Institut de Recherches Subatomiques (IN2P3-CNRS-Universite
Louis Pasteur), Strasbourg */
/* '5' Institute of Experimental Physics */
/* '6' Department of Physics */
/* '7' Institute of Physics and Astronomy */
/* '8' Kernfysisch Versneller Instituut, NL-9747 AA */
/* '9' SPring-8 */
REF=EPJ/A;
VLP=13(2002)411;
RCTS=58NI(3HE,T)58CU;
PHQS=TRNSN-STRGTH'10';
/* '10' Gamow-Teller transition probability B(GT) */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,1;
/* 2003-07-21 : Compiled */
RTY=RRG-RCT;
PHQ=TRNSN-STRGTH'11';
/* '11' Gamow-Teller transition probability B(GT) */
ENR=NAT;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=1.5MG/CM**2;
BAC=X;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC'12';
/* '12' RCNP Ring Cyclotron */
INST-ACC=2JPNRCN;
INC-ENGY-LAB=150MEV/A;
BEAM-INTNSTY=5NA;
CHRG-INC-ION=2+;
POL-PRJ=0%;
DET-PARTCL=T;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MWPC,MAG'13');
/* '13' The 3He2+ beam stopped in a Faraday cup inside the first
dipole magnet of the spectrometer which was set at 0 deg.. The
ejectile tritons were accepted with the full acceptance of the
spectrometer. */
SOLID-ANGL=XMSR'14';
/* '14' The spectrum was obtained around 0 deg. for the angular
range +-12 mr in the x-direction and no cut is made in the
y-direction. */
ERS-DET=50KEV'15';
/* '15' FWHM */
CALB-DET=/ The excitation energies of newly observed states were
calibrated using well-known low-lying discrete states of
12N and 13N [see ref. Nucl.Phys.A523(1991),1] observed in
the 0C(3He,t) spectrum as reference. /;
ANL=(DWBA'16',SHELL-MODEL);
/* '16' The authors use DWBA in order to evaluate thir data. DWBA
calculation was performed by using the code DW18 [by
J.R.Comfort]. The optical potential parameters for 3He were
taken from ref.[T.Yamagata et al., Nucl.Phys. A589(1995),425].
RCT=58NI(3HE,T)58CU;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
INC-ENGY-LAB=150MEV/A;
EMT=T;
RSD=58CU;
THTL=0DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY'17' TRNSN-STRGTH'18' DELTA-TRNSN-STRGTH'18,19' ISOSPIN
FLAG'20'
(MEV) (NODIM) (NODIM) (NODIM) (NODIM)
0.0 0.155 +-0.001 X 1.
0.204 X +-X 1 X
0.444 X +-X X X
1.051 0.265 +-0.013 X X
1.427 X +-X X X
1.651 X +-X X X
2.949 0.025 +-0.003 X X
3.460 0.173 +-0.011 X X
3.678 0.155 +-0.010 X X
3.717 0.050 +-0.005 X X
4.720 0.042 +-0.004 X X
5.065 0.040 +-0.004 X X
5.160 0.250 +-0.014 X X
5.451 0.082 +-0.007 X X
5.645 0.016 +-0.003 X X
6.038 0.029 +-0.004 X X
6.086 0.033 +-0.004 X X
6.497 0.061 +-0.007 X X
6.844 0.044 +-0.005 X X
7.105 0.057 +-0.006 X X
7.143 0.014 +-0.004 X X
7.586 0.073 +-0.007 1 X
7.700 0.021 +-0.004 X X
7.752 0.028 +-0.005 X X
7.907 0.052 +-0.005 1 X
7.993 0.049 +-0.005 X X
8.063 0.035 +-0.005 1? 3.
8.159 0.037 +-0.005 X 2.
8.199 0.033 +-0.004 X 2.
8.282 0.016 +-0.004 X 2.
\END;
/*===================================================================*/
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