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/* NRDF D0149 Data No.4 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,4;
D#=D149;
TITLE=/ The M1 transition strength from the 3/2- isobaric analogue
state in 49Sc /;
PURPOSE=/ To investigate the energetically impossible Gamow-Teller
beta transition by means of the corresponding M1 gamma decay
of the isobaric analogue state /;
ATH=(M.ADACHI'1', H.TAKETANI'1');
INST-ATH=(2JPNTIT'1');
/* '1' Department of Applied Physics */
REF=JPJ;
VLP=35(1973)325;
RCTS=(48CA(P,N)48SC, 48CA(P,GAMMA)49SC);
PHQS=(EXC-FUNCT, WDTH);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,4;
/* 2005-07-22 : Converted, Am + On, Converted to EXFOR E0149 */
POL-TGT=0%;
ALGN-TGT=0%;
ACC=VDG;
INST-ACC=2JPNTIT;
POL-PRJ=0%;
DET-PARTCL=GAMMA;
COINC=NO;
ANT-COINC=NO;
/* Related references
- M.Adachi et al., JPJ, 35(1973)317.
(Spin and parity taken from this reference)
RCT=48CA(P,GAMMA)49SC;
PHQ=WDTH;
INC-ENGY-LAB=1.93[2.01MEV;
DET-SYS=GE(LI)'2';
/* '2' To measure gamma rays */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,4;
TOT-ERR=X%'3';
/* '3' The uncertainties on the Gamma(gamma) are dominated by the
uncertainties on Gamma(n), which sum up to about 30% in the
cases of 1964- and 1975-keV resonances. In other three
resonances, the uncertainties on the Gamma(gamma) are due to
the uncertainties on Gamma(n) and intensities of gamma rays.
The uncertainty on the individual Gamma(gamma) ranged from 20
to 100%. */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
RESN-ENGY DELTA-RESN-ENGY EXC-ENGY-FINAL WDTH FLAG'4'
(KEV) (KEV) (KEV) (EV*10**-3) (NODIM)
1959.6 +-0.5 0 5 1
1959.6 +-0.5 2226 16 2
1959.6 +-0.5 2371 25 3
1959.6 +-0.5 3082 10 4
1959.6 +-0.5 3515 23 5
1959.6 +-0.5 3804 22 6
1959.6 +-0.5 3991 27 X
1959.6 +-0.5 4068 25 7
1959.6 +-0.5 4736 40 9
1959.6 +-0.5 6306 38 10
1959.6 +-0.5 6412 71 X
1959.6 +-0.5 6504 58 11
1959.6 +-0.5 6728 87 12
1959.6 +-0.5 6984 69 13
1959.6 +-0.5 7062 59 14
1959.6 +-0.5 7192 58 15
1959.6 +-0.5 7226 41 16
1964.2 +-0.7 2226 66 2
1964.2 +-0.7 2371 36 3
1964.2 +-0.7 3082 85 4
1964.2 +-0.7 3515 81 5
1964.2 +-0.7 3804 63 6
1964.2 +-0.7 3991 51 X
1964.2 +-0.7 4068 156 7
1964.2 +-0.7 4491 69 8
1964.2 +-0.7 4736 80 9
1964.2 +-0.7 6306 71 10
1964.2 +-0.7 6412 124 X
1964.2 +-0.7 6504 196 11
1964.2 +-0.7 6728 214 12
1964.2 +-0.7 6984 303 13
1964.2 +-0.7 7062 160 14
1964.2 +-0.7 7192 118 15
1964.2 +-0.7 7226 131 16
1974.7 +-0.5 0 127 1
1974.7 +-0.5 2226 82 2
1974.7 +-0.5 2371 59 3
1974.7 +-0.5 3082 34 4
1974.7 +-0.5 3515 58 5
1974.7 +-0.5 3804 146 6
1974.7 +-0.5 3991 147 X
1974.7 +-0.5 4068 259 7
1974.7 +-0.5 4491 78 8
1974.7 +-0.5 4736 182 9
1974.7 +-0.5 6306 67 10
1974.7 +-0.5 6412 292 X
1974.7 +-0.5 6504 538 11
1974.7 +-0.5 6728 431 12
1974.7 +-0.5 6984 593 13
1974.7 +-0.5 7062 331 14
1974.7 +-0.5 7192 246 15
1974.7 +-0.5 7226 268 16
1982.0 +-0.7 0 4 1
1982.0 +-0.7 2226 3 2
1982.0 +-0.7 2371 4 3
1982.0 +-0.7 3082 5 4
1982.0 +-0.7 3515 16 5
1982.0 +-0.7 3804 16 6
1982.0 +-0.7 3991 14 X
1982.0 +-0.7 4068 39 7
1982.0 +-0.7 4736 43 9
1982.0 +-0.7 6306 42 10
1982.0 +-0.7 6412 55 X
1982.0 +-0.7 6504 66 11
1982.0 +-0.7 6728 64 12
1982.0 +-0.7 6984 40 13
1982.0 +-0.7 7062 34 14
1982.0 +-0.7 7192 28 15
1982.0 +-0.7 7226 48 16
1991.3 +-1.0 2226 6 2
1991.3 +-1.0 3082 28 4
1991.3 +-1.0 3515 29 5
1991.3 +-1.0 3804 48 6
1991.3 +-1.0 3991 34 X
1991.3 +-1.0 4068 54 7
1991.3 +-1.0 4736 30 9
1991.3 +-1.0 6306 40 10
1991.3 +-1.0 6412 31 X
1991.3 +-1.0 6504 53 11
1991.3 +-1.0 6728 42 12
1991.3 +-1.0 6984 36 13
1991.3 +-1.0 7062 41 14
1991.3 +-1.0 7192 26 15
1991.3 +-1.0 7226 42 16
\END;
/*===================================================================*/
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