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 /* NRDF D1620 Data No.7                                              */
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 /* Bibliography                                                      */
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 \\BIB,7;
 D#=D1620;
 TITLE=/ Strength functions of deeply bound hole states in 111, 115,
         119, 123Sn /;
 PURPOSE=/ To investigate the strength functions of deeply bound hole
           states in 111, 115, 119, 123Sn nuclei with high resolution
           (p,d) experiments at the bombaring energy of 50 MeV. /;
 ATH=(M.MATOBA'1', H.IJIRI'1', H.KAMETANI'1', I.KUMABE'2',
      M.HYAKUTAKE'2', N.KOORI'2', T.SAKAE'2', T.MAKI'3');
 INST-ATH=(2JPNKYU'1', 2JPNKYU'2', 2JPNKIT'3');
      /* '1' Graduate School of Engineering Sciences */
      /* '2' Faculty of Engineering */
      /* '3' School of Nursing and Technology */
 REF=NP/A;
 VLP=456(1986)235;
 RCTS=(112SN(P,D)111SN, 124SN(P,D)123SN, 116SN(P,D)115SN,
       120SN(P,D)119SN);
 PHQS=(ANGL-DSTRN, SPEC-FCTR'4');
 /* '4' The spectroscopic factors as a function of the average
    excitation energies */
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 /* Experimental Conditions                                           */
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 \\EXP,7;
 /* 2003-10-02 : Converted, Sr + Am + On. Converted to EXFOR E1620
 RTY=PKUP;
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB=50.4MEV;
 POL-PRJ=0%;
 DET-PARTCL=D;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'5',X'6');
 /* '5' Multi-magnet spectrograph RAIDEN [H.Ikegami et al., Nucl.
        Instr. Meth. 175(1980)33] */
 /* '6' Focal plane detector system KYUSHU [M.Matoba et al., Nucl.
        Instr. Meth. 180(1981)419] */
 RCT=112SN(P,D)111SN;
 PHQ=SPEC-FCTR'8';
 /* '8' The spectroscopic factors as a function of the average
        excitation energies */
 ENR=80.04%;
 THK-TGT=0.9MG/CM**2;
 ANL=X'9';
 /* '9' Theoretical predictions by Soloviev et al. [V.G.Soloviev et
        al.,Nucl.Phys.A342(1980)261;N.D.Thao et al.,
        Yadr.Phys.34(1983)43] */
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 /* Descriptive Parameters                                            */
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 \\DATA,7;
 INC-ENGY-LAB=50.4MEV;
 SYS-ERR=<20%'7';
 /* '7' The accuracy of the normalization of the absolute cross
        section is better than 20% */
 NORM=/ The absolute (p,d) cross sections were obtained by
        normalization to proton elastic scattering measured under
        identical experimental conditions, except for magnetic field
        adjustment of the spectrograph. /;
 SYS-ERR=([20%'10',X%'11');
 /* '10' The errors of the deduced spectroscopic factors are
         estimated to be about 20% due mainly to the absolute
         normalization procedure. */
 /* '11' The errors of the excitation energies and spreading
         widths may be small because the error of the absolute cross
         section only weakly affects the final results. */
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 /* Data Table                                                        */
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 \DATA;
 EXC-ENGY'12' SPEC-FCTR WDTH'13' L'14'
 (MEV) (NODIM) (MEV) (NODIM)
 4.09 5.38 1.05 4
 5.06 2.18 2.41 1
 5.11 8.87 3.48 4
 5.98 3.25 3.78 1
 6.67 3.49 2.65 4
 7.86 1.06 1.62 1
 \END;
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