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/* NRDF D1523 Data No.21 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,21;
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,21;
/* 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,21;
INC-ENGY-LAB=65MEV;
SYS-ERR=X%'80';
/* '80' Uncertainty in run-to-run variations of the integrated
beam current are on the order of a few percent. */
EMT=D;
EXC-ENGY=0.656MEV;
J-PTY=1/2-;
TRNSF-L=1'81';
/* '81' Transferred orbital angular momentum (L) */
TRNSF-J=1/2'82';
/* '82' Transferred total angular momentum (J) */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC AY DELTA-AY
(DEG) (NODIM) (NODIM)
4.887E+00 -4.230E-01 +-2.902E-02
8.009E+00 -2.251E-01 +-3.348E-02
1.079E+01 1.136E-01 +-3.571E-02
1.409E+01 4.365E-01 +-4.241E-02
1.706E+01 2.327E-01 +-4.464E-02
1.999E+01 3.780E-02 +-4.911E-02
2.315E+01 -8.769E-04 +-4.241E-02
2.645E+01 4.537E-01 +-4.018E-02
2.927E+01 6.740E-01 +-4.687E-02
3.246E+01 4.858E-01 +-4.687E-02
3.521E+01 1.638E-01 +-6.250E-02
4.053E+01 1.692E-01 +-6.250E-02
4.557E+01 6.993E-01 +-6.473E-02
\END;
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