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/* NRDF D1523 Data No.69 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,69;
D#=D1523;
TITLE=/ Hole strengths and spreading widths observed in
92Mo(p,d)91Mo reaction at 65 MeV /;
PURPOSE=/ To assign spin-parities and determine spectroscopic
factors of excited neutron-hole states of 91Mo nuclei in the
excitation energy region of 0-10 MeV /;
ATH=(K.HISAMOCHI'1', O.IWAMOTO'1', A.KISANUKI'1', S.BUDIHARDJO'1',
S.WIDODO'1', A.NOHTOMI'1', Y.UOZUMI'1', T.SAKAE'1', M.MATOBA'1',
M.NAKANO'2', T.MAKI'2', S.MATSUKI'3', N.KOORI'4');
INST-ATH=(2JPNKYU'1', 2JPNKIT'2', 2JPNKTO'3', 2JPNTKS'4');
/* '1' Faculty of Engineering */
/* '2' School of Nursing and Technology */
/* '3' Chemical Research Institute */
/* '4' College of General Education */
REF=NP/A;
VLP=564(1993)227;
RCTS=92MO(P,D)91MO;
PHQS=(ANGL-DSTRN, VCTR-ANALPW, SPEC-FCTR);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,69;
/* 2005-10-12 : Converted, Kc + Sr + On. Converted to EXFOR E523
/* 2005-11-12 : Altered, On + Kc + Sr. Re-digitized */
ENR=X%'5';
/* '5' Enriched target */
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=0.506MG/CM**2;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC'6';
/* '6' Isochronous cyclotron, AVF cyclotron */
INST-ACC=2JPNRCN;
INC-ENGY-LAB=65MEV;
POL-PRJ=X%'7';
/* '7' A polarized proton beam was used */
DET-PARTCL=D;
COINC=NO;
ANT-COINC=NO;
DET-SYS=MAG'8';
/* '8' Spectrograph RAIDEN [H. Ikegami et al., Nucl. Instr. Meth.
175(1980)33] viewed with the focal plane detector system KYUSHU
[M. Matoba et al., Nucl. Instr. Meth. 180(1980)419] */
ERS-DET=40KEV;
ANL=DWBA;
RCT=92MO(P,D)91MO;
PHQ=SPEC-FCTR;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,69;
INC-ENGY-LAB=65MEV;
SYS-ERR=X%'247';
/* '247' Uncertainty in run-to-run variations of the integrated
beam current are on the order of a few percent. */
EMT=D;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY TRNSF-L TRNSF-J'248' SPEC-FCTR
(MEV) (NODIM) (NODIM) (NODIM)
0.000 4 9/2 6.092
0.656 1 1/2 1.575
1.158 1 3/2 1.759
1.365 2 5/2 0.118
1.532 3 5/2 2.319
1.902 4 9/2 0.508
2.084 1 3/2 0.159
2.226 4 9/2 0.068
2.304 4 9/2 0.401
2.304 1 1/2 0.0456
2.454 4 9/2 0.101
2.718 3 5/2 0.733
2.821 4 9/2 0.406
2.901 1 3/2 0.147
3.187 1 3/2 0.0791
3.330 4 9/2 0.271
3.456 3 7/2 0.922
3.591 3 7/2 0.197
3.649 2 5/2 0.0314
3.823 3 7/2 0.339
3.956 4 9/2 0.170
3.956 3 7/2 0.0729
4.074 4 9/2 0.244
4.151 3 7/2 0.139
4.151 4 9/2 0.135
4.283 4 9/2 0.203
4.383 3 7/2 0.148
4.383 3 5/2 0.109
4.481 3 5/2 0.235
4.664 1 3/2 0.176
4.796 3 7/2 0.490
5.295 3 7/2 0.255
5.394 3 7/2 0.535
5.516 3 7/2 0.657
5.690 3 7/2 0.431
5.930 3 7/2 0.691
6.070 3 7/2 0.581
7.026 4 9/2 0.229
7.158 1 1/2 0.246
8.433 1 3/2 0.183
8.742 1 3/2 0.257
8.938 3 5/2 0.679
\END;
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