/*===================================================================*/
 /* NRDF D1913 Data No.7                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,7;
 D#=D1913;
 TITLE=/ The 96Mo(p,d)95Mo reaction at 50 MeV /;
 ATH=(S.A.SULTANA'1', D.MAKI'1', G.WAKABAYASHI'1', Y.UOZUMI'1',
      N.IKEDA'1', SYAFARUDIN'2', F.ARAMAKI'3', T.KAWAGUCHI'4',
      M.MATOBA'4', H.M.SEN GUPTA'5');
 INST-ATH=(2JPNKYU'1', 3INSINS'2', 2JPNJPN'3', 2JPNJPN'4', 3BANDAC'5');
      /* '1' Department of Applied Quantum Physics and Nuclear
            Engineering */
      /* '2' P2TKN-BATAN, Kawasan PUSPIPTEK Serpong */
      /* '3' Kyushu Institute of Information Sciences, Dazaifu */
      /* '4' Faculty of Engineering, Kyushu Sangyo University, Fukuoka
      /* '5' Department of Physics */
 REF=PR/C;
 VLP=70(2004)034612;
 RCTS=96MO(P,D)95MO;
 PHQS=(ANGL-DSTRN, VCTR-ANALPW, DBL-DIFF-XSECTN);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,7;
 /* 2005-09-14 : Deleted, Kc + On */
 /* Related references 
    - J.J.Menet et al., PR/C, 4(1971)1114.
    (Absolute cross sections are obtained by scaling the measured
    p+96Mo elastic scattering cross section to the optical model
    prediction at small angles using the global potential given in this
    reference.)
 ENR=[98%'6';
 /* '6' Isotopically enriched target */
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.79MG/CM**2;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'7';
 /* '7' Isochronous cyclotron, AVF Cyclotron */
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB=50MEV;
 POL-PRJ=X%;
 DET-PARTCL=D;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'8',X'9');
 /* '8' For momentum analysis using RAIDEN [H. Ikegami, et al.,
        Nucl. Instrum. Methods 175(1980)335] */
 /* '9' Focal plane detector system KYUSHU [M. Matoba et al., Nucl.
        Instrum. Methods 180(1981)419]. */
 ERS-DET=40KEV'10';
 /* '10' Full width at half maximum (FWHM) */
 CALB-DET=/ Energy is calibrated by remapping some positions of
            well-known low-lying levels in 95Mo, the ground state,
            0.766, 0.821, 0.948, and 1.048 (average of 1.039 and 1.057)
            MeV [R. B. Firestone et al., Table of Isotopes, 8th ed.
            (Wiley, New York, 1996 )] /;
 ANL=DWBA'11';
 /* '11' Zero range DWBA code DWUCK-4 */
 /* Comment to data: Author's comment: J-pi assignments are doubtful
    for the following levels (MeV): 1.049, 1.356, 1.916, 2.152, 2.223,
    3.162, 3.264, 4.032, 4.299, 4.394, 4.486, 4.533, 4.792, 4.860,
    4.908 */
 RCT=96MO(P,D)95MO;
 PHQ=ANGL-DSTRN;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,7;
 INC-ENGY-LAB=50MEV;
 EXC-ENGY=3.264MEV;
 J-PTY=3/2+;
 TRNSF-L=2'24';
 /* '24' Transferred angular momentum L */
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA'25'
 (DEG) (MB/SR) (MB/SR)
 8.1386 0.336 +-0.0216
 11.187 0.301 +-0.0195
 14.235 0.2 +-0.0148
 17.283 0.135 +-0.0105
 20.33 0.101 +-0.00804
 23.376 0.0696 +-0.00505
 26.42 0.0664 +-0.00513
 29.464 0.0553 +-0.00406
 33.52 0.0304 +-0.00248
 38.587 0.0221 +-0.0021
 43.65 0.0234 +-0.00181
 48.708 0.0143 +-0.00135
 \END;
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