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 /* NRDF D1913 Data No.40                                             */
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 /* Bibliography                                                      */
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 \\BIB,40;
 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,40;
 /* 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=VCTR-ANALPW;
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,40;
 INC-ENGY-LAB=50MEV;
 EXC-ENGY=0.948MEV;
 J-PTY=9/2+;
 TRNSF-L=4'90';
 /* '90' Transferred angular momentum L */
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 /* Data Table                                                        */
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 \DATA;
 THTC AY DELTA-AY'91'
 (DEG) (NODIM) (NODIM)
 8.1386 0.1167 +-0.078593
 11.187 -0.003372 +-0.082058
 14.235 0.008486 +-0.079882
 17.283 -0.02227 +-0.073312
 20.33 0.015298 +-0.075843
 23.376 0.033869 +-0.07717
 26.42 0.081259 +-0.079032
 29.464 0.047745 +-0.080586
 33.52 -0.31774 +-0.085129
 38.587 0.056263 +-0.084663
 43.65 -0.083396 +-0.086774
 48.708 -0.019087 +-0.094207
 \END;
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