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 /* NRDF D1305 Data No.20                                             */
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 /* Bibliography                                                      */
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 \\BIB,20;
 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,20;
 /* 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)99MO/237NP(P,FISSN)97NB);
 PHQ=EXC-FUNCT;
 INC-ENGY-LAB=9[32MEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,20;
 EMT=GAMMA'37';
 /* '37' Decay data not given */
 RSD=(99MO,97NB);
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-LAB XSECTN-RATIO DELTA-XSECTN-RATIO
 (MEV) (NODIM) (NODIM)
 1.368E+01  1.030E+00  +-3.012E-01
 1.424E+01  1.045E+00  +-1.531E-01
 1.482E+01  7.678E-01  +-1.826E-01
 1.531E+01  9.074E-01  +-1.968E-01
 1.598E+01  9.016E-01  +-1.766E-01
 1.684E+01  8.025E-01  +-7.442E-02
 1.717E+01  6.373E-01  +-1.289E-01
 1.753E+01  8.424E-01  +-NEGLIGIBLE
 1.802E+01  9.624E-01  +-NEGLIGIBLE
 1.821E+01  8.084E-01  +-NEGLIGIBLE
 1.835E+01  8.290E-01  +-NEGLIGIBLE
 1.865E+01  7.367E-01  +-NEGLIGIBLE
 1.913E+01  9.173E-01  +-NEGLIGIBLE
 1.945E+01  9.387E-01  +-NEGLIGIBLE
 2.044E+01  6.886E-01  +-NEGLIGIBLE
 2.182E+01  6.072E-01  +-NEGLIGIBLE
 2.265E+01  6.181E-01  +-NEGLIGIBLE
 2.360E+01  6.374E-01  +-NEGLIGIBLE
 2.454E+01  6.775E-01  +-NEGLIGIBLE
 2.728E+01  3.244E-01  +-NEGLIGIBLE
 2.843E+01  5.304E-01  +-NEGLIGIBLE
 2.954E+01  5.776E-01  +-NEGLIGIBLE
 3.031E+01  5.315E-01  +-NEGLIGIBLE
 3.121E+01  4.933E-01  +-NEGLIGIBLE
 3.222E+01  5.119E-01  +-NEGLIGIBLE
 3.550E+01  2.436E-01  +-NEGLIGIBLE
 \END;
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