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 /* NRDF D1523 Data No.25                                             */
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 /* Bibliography                                                      */
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 \\BIB,25;
 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                                           */
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 \\EXP,25;
 /* 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=ANGL-DSTRN;
 MONTR-RCT=/ 92MO(P,P)92MO /;
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 /* Descriptive Parameters                                            */
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 \\DATA,25;
 INC-ENGY-LAB=65MEV;
 SYS-ERR=(<25%'94',X%'95');
 /* '94' Total systematic error. Mainly due to the ambiguity of
         the procedure for fitting the theoretical to the experimental
         angular distributions */
 /* '95' Uncertainty in run-to-run variations of the integrated
         beam current are on the order of a few percent. */
 EMT=D;
 EXC-ENGY=2.901MEV;
 J-PTY=3/2-;
 TRNSF-L=1'96';
 /* '96' Transferred orbital angular momentum (L) */
 TRNSF-J=3/2'97';
 /* '97' Transferred total angular momentum (J) */
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 /* Data Table                                                        */
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 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (MB/SR) (MB/SR)
 4.859E+00 4.139E-01 +-7.103E-02
 7.733E+00 2.847E-01 +-2.916E-02
 1.073E+01 1.786E-01 +-2.071E-02
 1.394E+01 1.456E-01 +-1.104E-02
 1.677E+01 1.217E-01 +-1.164E-02
 1.982E+01 1.362E-01 +-9.440E-03
 2.310E+01 1.111E-01 +-7.696E-03
 2.591E+01 7.731E-02 +-5.862E-03
 2.917E+01 4.940E-02 +-4.397E-03
 3.224E+01 3.566E-02 +-3.412E-03
 3.520E+01 5.753E-02 +-4.741E-03
 4.039E+01 3.559E-02 +-3.405E-03
 4.535E+01 2.742E-02 +-2.079E-03
 \END;
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