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 /* NRDF D1853 Data No.3                                              */
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 /* Bibliography                                                      */
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 \\BIB,3;
 D#=D1853;
 TITLE=/ Mass separation of neutron-rich isotopes using a gas-jet
         coupled thermal ion source /;
 PURPOSE=/ To report on the design and performance of the gas-jet
           coupled thermal ion source installed in the JAERI-ISOL /;
 ATH=(S.ICHIKAWA'1', M.ASAI'2', K.TSUKADA'1', A.OSA'3', T.IKUTA'2',
      N.SHINOHARA'1', H.IIMURA'1', Y.NAGAME'1', Y.HATSUKAWA'1',
      I.NISHINAKA'1', K.KAWADE'4', H.YAMAMOTO'4', M.SHIBATA'4',
      Y.KOJIMA'4');
 INST-ATH=(2JPNJAE'1', 2JPNNAG'2', 2JPNJAE'3', 2JPNNAG'4');
      /* '1' Department of Radioisotopes */
      /* '2' Department of Nuclear Engineering */
      /* '3' Department of Radioisotopes (Takasaki Establishment) */
      /* '4' Department of Energy Engineering and Science */
 REF=NIM/A;
 VLP=374(1996)330;
 RCTS=(238U(P,FISSN), 238U(P,FISSN)140CS, 238U(P,FISSN)144CS,
       238U(P,FISSN)144BA, 238U(P,FISSN)144LA, 238U(P,FISSN)148LA,
       238U(P,FISSN)148CE, 238U(P,FISSN)148PR, 238U(P,FISSN)152ND,
       238U(P,FISSN)156PM, 238U(P,FISSN)160EU);
 PHQS=XSECTN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,3;
 /* 2003-11-05 : Converted, R.Suzuki + N.Otuka. Data converted from
    EXFOR O0747 */
 RTY=FISSN;
 PHQ=XSECTN;
 /* Additional results shown but not compiled
    - The first observation of a new isotope 166Tb was carried out
      using its monoxide ions. Half-life of 166Tb is 21+-6 sec.
      Separation efficiency was reported.
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=1.1MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNJAE;
 INC-ENGY-LAB-RANGE=15MEV;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 /* Experimental Method:
    - On-line mass separation (Gas-jet coupled thermal ion source was
      installed in the isotope separator on line.)
    - Gamma ray spectrometry
 /* By authors: Reaction yield was evaluated by the reaction cross
    section and correction made, if necessary for the charge
    distribution by assuming a Gaussian charge distribution with the
    most probable distribution Z(p) of the unchanged charge
    distribution model. */
 RCT=238U(P,FISSN)144CS;
 DET-PARTCL=GAMMA'8';
 /* '8' Delayed gamma from 144Cs (ground state)Abundance is less
        than 47% */
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 /* Descriptive Parameters                                            */
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 \\DATA,3;
 INC-ENGY-LAB=15MEV;
 ENGY-GAMMA=199.3KEV'9';
 INTNSTY-GAMMA=0.47'9';
 HALF-LIFE=1.02SEC'9';
 /* '9' Delayed gamma from 144Cs (ground state) (Abundance is less
        than 47%) */
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 /* Data Table                                                        */
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 \DATA;
 XSECTN
 (MB)
 0.49
 \END;
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