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 /* NRDF D1685 Data No.27                                             */
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 /* Bibliography                                                      */
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 \\BIB,27;
 D#=D1685;
 TITLE=/ (p,d) reaction on 62Ni at 65 MeV /;
 PURPOSE=/ To restudy this type of reactions with a high
           resolutionpolarized beam and magnetic spectrograph system /;
 ATH=(M.MATOBA'1', K.KUROHMARU'1', O.IWAMOTO'1', A.NOHTOMI'1',
      Y.UOZUMI'1', T.SAKAE'1', N.KOORI'2', H.OHGAKI'3', H.IJIRI'3',
      T.MAKI'4', M.NAKANO'4', H.M.SEN GUPTA'5');
 INST-ATH=(2JPNKYU'1', 2JPNTKS'2', 2JPNKYU'3', 2JPNKIT'4',
           3BANDAC'5');
      /* '1' Department of Nuclear Engineering */
      /* '2' Faculty of Integrated Arts and Sciences */
      /* '3' Graduate School of Engineering Sciences */
      /* '4' School of Nursing and Technology */
      /* '5' Department of Physics */
 REF=PR/C;
 VLP=53(1996)1792;
 RCTS=62NI(P,D)61NI;
 PHQS=(ANGL-DSTRN, VCTR-ANALPW);
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 /* Experimental Conditions                                           */
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 \\EXP,27;
 /* 2003-09-10 : Converted, Am + On. Data converted to EXFOR E1685
 RTY=PKUP;
 ENR=99.7%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.491MG/CM**2;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'6';
 /* '6' Isochronous cyclotron, AVF cyclotron facility */
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB=65MEV;
 POL-PRJ=X%;
 ION-SOURCE=/ Polarized ion source (Value of beam polarization is not
              given in the reference.) /;
 DET-PARTCL=D;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'7',X'8');
 /* '7' Emitted deuterons were detected in the focal plane of the
        spectrograph (RAIDEN)[H.Ikegami et al., Nucl. Instrm. Methods
        175, 33(1980)] */
 /* '8' Emitted deuterons were viewed with the focal plane detector
        system KYUSHU[M.Matoba et al.,Nucl. Instrm. Methods
        180,419(1981)] */
 /* 2006-11-09 : Altered, At. Re-digitized */
 RCT=62NI(P,D)61NI;
 PHQ=VCTR-ANALPW;
 ANL=DWBA;
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 /* Descriptive Parameters                                            */
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 \\DATA,27;
 INC-ENGY-LAB=65MEV;
 NORM=/ The normalization of the cross section is performed by scaling
        the measured p+62Ni elastic scattering cross section to an
        optical model prediction using parameters of global potentials.
        [J.J.H. Menet et al., Phys. Rev. C 4, 1114 (1971); F.D.
        Becchetti, Jr. and G.W. Greenlees, Phys. Rev. 182, 1190 (1969)]
 EXC-ENGY=1.458MEV;
 J-PTY=7/2-;
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 /* Data Table                                                        */
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 \DATA;
 THTC AY DELTA-AY
 (DEG) (NODIM) (NODIM)
 5.720E+00 -4.247E-02 +-2.467E-02
 8.880E+00 3.497E-02 +-1.763E-02
 1.196E+01 1.159E-01 +-1.410E-02
 1.505E+01 1.652E-01 +-2.115E-02
 1.805E+01 1.157E-01 +-1.762E-02
 2.105E+01 2.046E-02 +-2.467E-02
 2.406E+01 9.787E-03 +-2.115E-02
 2.722E+01 -7.492E-02 +-2.820E-02
 3.038E+01 2.720E-02 +-2.820E-02
 3.338E+01 1.328E-01 +-2.467E-02
 3.654E+01 2.350E-01 +-2.820E-02
 3.962E+01 1.855E-01 +-3.173E-02
 4.271E+01 1.889E-01 +-3.172E-02
 4.679E+01 1.958E-01 +-3.172E-02
 \END;
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