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/* NRDF D1523 Data No.11 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,11;
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,11;
/* 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=VCTR-ANALPW;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,11;
INC-ENGY-LAB=65MEV;
SYS-ERR=X%'48';
/* '48' Uncertainty in run-to-run variations of the integrated
beam current are on the order of a few percent. */
EMT=D;
EXC-ENGY=1.902MEV;
J-PTY=9/2+;
TRNSF-L=4'49';
/* '49' Transferred orbital angular momentum (L) */
TRNSF-J=9/2'50';
/* '50' Transferred total angular momentum (J) */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC AY DELTA-AY
(DEG) (NODIM) (NODIM)
4.861E+00 -3.252E-03 +-9.061E-02
8.003E+00 2.159E-02 +-9.708E-02
1.084E+01 1.760E-01 +-9.385E-02
1.395E+01 2.017E-01 +-5.272E-02
1.712E+01 2.451E-01 +-5.825E-02
1.994E+01 8.233E-02 +-5.825E-02
2.314E+01 -3.200E-02 +-5.178E-02
2.622E+01 -6.650E-04 +-5.503E-02
2.898E+01 1.136E-02 +-5.501E-02
3.219E+01 4.265E-02 +-5.825E-02
3.533E+01 1.031E-01 +-7.119E-02
4.042E+01 5.932E-02 +-5.825E-02
4.519E+01 2.861E-02 +-8.090E-02
\END;
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