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 /* NRDF D1358 Data No.12                                             */
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 /* Bibliography                                                      */
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 \\BIB,12;
 D#=D1358;
 TITLE=/ Evaporation residue formation competing with the fission
         process in the 197Au+16O, 12C reactions and fission barriers
         at a specified J window /;
 ATH=(S.BABA'1', K.HATA'1', S.ICHIKAWA'1', T.SEKINE'1', Y.NAGAME'1',
      A.YOKOYAMA'2', M.SHOJI'2', T.SAITO'2', N.TAKAHASHI'2', H.BABA'2',
      I.FUJIWARA'3');
 INST-ATH=(2JPNJAE'1', 2JPNOSA'2', 2JPNJPN'3');
      /* '2' Department of Chemistry and Laboratory of Nuclear Studies
      /* '3' School of Economics, Otemon Gakin University, Osaka */
 REF=ZP/A;
 VLP=331(1988)53;
 RCTS=(197AU(16O,3*N)210FR, 197AU(16O,4*N)209FR, 197AU(16O,5*N)208FR,
       197AU(16O,6*N)207FR, 197AU(16O,7*N)206FR, 197AU(16O,FUSN),
       197AU(12C,FUSN), 197AU(12C,3*N)206AT, 197AU(12C,4*N)205AT,
       197AU(12C,5*N)204AT, 197AU(12C,6*N)203AT);
 PHQS=(EXC-FUNCT, EXC-FUNCT'4');
 /* '4' Evaporation residue cross section */
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 /* Experimental Conditions                                           */
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 \\EXP,12;
 /* 2006-05-23 : Converted, N.Otuka. Converted to EXFOR E1358 */
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=2.0MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNJAE;
 BEAM-INTNSTY=50PNA;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 /* 2006-08-02 : Altered, Is. Re-digitized */
 RCT=197AU(12C,3*N)206AT;
 PHQ=EXC-FUNCT;
 DET-PARTCL=GAMMA'44';
 /* '44' Delayed gamma from 206At */
 DET-SYS=(GE(LI)'45',HPGE'45');
 /* '45' To measure radioactivities */
 /* Experimental Method:
    - Activation (Irradiated for 10 min to 2 hour)
    - Gamma ray spectrometry (Measured over a few weeks)
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 /* Descriptive Parameters                                            */
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 \\DATA,12;
 ENGY-GAMMA=700.7KEV'46';
 INTNSTY-GAMMA=0.97'46';
 HALF-LIFE=31.4MIN'46';
 /* '46' Delayed gamma from 206At */
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-CM SIGMA DELTA-SIGMA
 (MEV) (MB) (MB)
 5.946E+01 6.181E+01 +-4.706E+00
 6.592E+01 2.108E+01 +-1.368E+00
 6.938E+01 9.325E+00 +-1.030E+00
 \END;
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