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 /* NRDF D1231 Data No.2                                              */
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 /* Bibliography                                                      */
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 \\BIB,2;
 D#=D1231;
 TITLE=/ Nucleon transfer in highly mass-asymmetric reaction systems
         between 197Au and relatively light projectiles in the energy
         region below 10 MeV/u I.Target-like products /;
 ATH=(A.YOKOYAMA'1', T.SAITO'1', M.SHOJI'1', H.BABA'1', S.BABA'2',
      K.HATA'2', T.SEKINE'2', S.ICHIKAWA'2');
 INST-ATH=(2JPNOSA'1', 2JPNJAE'2');
      /* '1' Department of Chemistry and Laboratory of Nuclear Studies
 REF=ZP/A;
 VLP=332(1989)61;
 RCTS=(197AU(37CL,X)X, 197AU(37CL,X)196AU, 197AU(16O,X)X,
       197AU(14N,X)X, 197AU(14N,X)196AU, 197AU(12C,X)X);
 PHQS=XSECTN;
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 /* Experimental Conditions                                           */
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 \\EXP,2;
 /* 2007-01-20 : Converted, N.Otuka. Converted to EXFOR E1231 */
 PHQ=XSECTN;
 /* Additional results shown but not compiled
    - Range of recoils measured (Shown in Fig.3-6 in reference)
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 POL-TGT=0%;
 ALGN-TGT=0%;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=GE(LI)'3';
 /* '3' To measure gamma rays from each foil of target stack */
 /* Experimental Method:
    - Stacked target irradiation (Several pairs of Au target foil and
      Al catcher foil)
    - Activation
    - Chemical separation (To detect small yields of Au isotopes)
 RCT=197AU(37CL,X)X'6';
 /* '6' See DATA section for atomic number (Z) and mass number (A)
        of products */
 ACC=VDGT;
 INST-ACC=2JPNJAE;
 INC-ENGY-LAB-RANGE=180MEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
 INC-ENGY-LAB=180MEV;
 TOT-ERR=X%'7';
 /* '7' Uncertainty in fitting process in decay analysis, gamma-ray
        branching ratio and statistical uncertainty */
 Z=79;
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 /* Data Table                                                        */
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 \DATA;
 A ISOMER SIGMA DELTA-SIGMA HALF-LIFE
 (NODIM) (NODIM) (MB) (MB) (SEC)
 198 0 4.97 +-0.02 233020.8
 196 0 21.8 +-0.6 534211.2
 196 1 0.44 +-0.04 34920
 195 0 6.4 +-1.4 15811200
 194 0 0.30 +-0.02 142200
 \END;
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