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 /* NRDF D1305 Data No.16                                             */
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 /* Bibliography                                                      */
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 \\BIB,16;
 D#=D1305;
 TITLE=/Systematic analysis of mass yield curves in low-energy fission
        of actinides/;
 ATH=(T.OHTSUKI'1', Y.HAMAJIMA'1', K.SUEKI'1', H.NAKAHARA'1',
      Y.NAGAME'2', N.SHINOHARA'2', H.IKEZOE'2');
 INST-ATH=(2JPNTMU'1', 2JPNJAE'2');
      /* '1' Department of Chemistry, Faculty of Science */
 REF=PR/C;
 VLP=40(1989)2144;
 RCTS=(233U(P,FISSN), 235U(P,FISSN), 237NP(P,FISSN), 238U(P,FISSN),
       239PU(P,FISSN), 242PU(P,FISSN), 244PU(P,FISSN), 241AM(P,FISSN),
       243AM(P,FISSN), (P,FISSN), 237NP(P,FISSN)85KR,
       237NP(P,FISSN)97NB, 237NP(P,FISSN)87KR, 237NP(P,FISSN)88KR,
       237NP(P,FISSN)91SR, 237NP(P,FISSN)92SR, 237NP(P,FISSN)93Y,
       237NP(P,FISSN)95ZR, 237NP(P,FISSN)99MO, 237NP(P,FISSN)103RU,
       237NP(P,FISSN)105RH, 237NP(P,FISSN)111AG, 237NP(P,FISSN)112PD,
       237NP(P,FISSN)113AG, 237NP(P,FISSN)115CD, 237NP(P,FISSN)117CD,
       237NP(P,FISSN)126SB);
 PHQS=(A-DSTRN, DATA'3', DATA'4', DATA'5', EXC-FUNCT);
 /* '3' Weighted mean peak positions of heavy asymmetric peak */
 /* '4' Weighted mean peak positions of light asymmetric peak */
 /* '5' Full width at half maximum of asymnetric peak */
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 /* Experimental Conditions                                           */
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 \\EXP,16;
 /* 2004-03-25 : Converted, Data converted to EXFOR E1305 */
 RTY=(FISSN,FISSN,FISSN);
 ENR=>99%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.100[0.300MG/CM**2'6';
 /* '6' Thickness was determined by alpha spectrometry */
 BAC=AL'7';
 /* '7' Electrodeposited on Al foil and wrapped with a sheet of Al
        foil */
 THK-BAC=6MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(VDGT'8',CYC'9');
 /* '9' Isochronous cyclotron */
 INST-ACC=(2JPNJAE'8',2JPNINS'9');
 BEAM-INTNSTY=[1UA;
 POL-PRJ=0%;
 DET-PARTCL=GAMMA'10';
 /* '10' . Decay data not given */
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=GE(LI)'11';
 /* '11' To detect decay gamma */
 /* Experimental Method:
    - Activation
 /* Analysis:
    - Mass yield curves were constructed from the observed cross
      section of each fission product to which a correction was
      applied, when necessary, for the charge distribution by assuming
      a Gaussian charge distribution with the most probable charge Zp
      of unchanged-charge division. The Gaussian width parameter of
      0.95 was used as suggested by McHugh et al. [J.A. Mchugh and M.C.
      Michel, Phys. ReV. 172(1968)1160].
 RCT=(237NP(P,FISSN)91SR/237NP(P,FISSN)97NB);
 PHQ=EXC-FUNCT;
 INC-ENGY-LAB=9[32MEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,16;
 EMT=GAMMA'33';
 /* '33' Decay data not given */
 RSD=(91SR,97NB);
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-LAB XSECTN-RATIO DELTA-XSECTN-RATIO
 (MEV) (NODIM) (NODIM)
 9.780E+00  4.724E-01  +-1.120E-01
 1.041E+01  4.829E-01  +-9.077E-02
 1.096E+01  5.447E-01  +-1.089E-01
 1.155E+01  5.645E-01  +-9.174E-02
 1.220E+01  6.335E-01  +-8.365E-02
 1.267E+01  4.644E-01  +-9.771E-02
 1.298E+01  4.612E-01  +-9.509E-02
 1.325E+01  5.905E-01  +-NEGLIGIBLE
 1.344E+01  6.769E-01  +-NEGLIGIBLE
 1.383E+01  6.720E-01  +-1.241E-01
 1.431E+01  6.577E-01  +-NEGLIGIBLE
 1.471E+01  7.073E-01  +-NEGLIGIBLE
 1.529E+01  6.386E-01  +-1.380E-01
 1.569E+01  5.671E-01  +-1.257E-01
 1.682E+01  5.451E-01  +-8.526E-02
 1.784E+01  4.015E-01  +-8.001E-02
 1.886E+01  4.999E-01  +-1.080E-01
 1.949E+01  5.319E-01  +-9.183E-02
 2.043E+01  5.522E-01  +-6.212E-02
 2.175E+01  5.542E-01  +-8.878E-02
 2.286E+01  6.865E-01  +-1.268E-01
 2.388E+01  5.728E-01  +-9.006E-02
 2.478E+01  4.223E-01  +-6.679E-02
 2.551E+01  5.633E-01  +-6.881E-02
 2.645E+01  4.599E-01  +-NEGLIGIBLE
 2.786E+01  4.844E-01  +-NEGLIGIBLE
 2.954E+01  5.564E-01  +-NEGLIGIBLE
 3.196E+01  5.464E-01  +-5.679E-02
 \END;
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