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 /* NRDF D1305 Data No.19                                             */
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 /* Bibliography                                                      */
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 \\BIB,19;
 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,19;
 /* 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)95ZR/237NP(P,FISSN)97NB);
 PHQ=EXC-FUNCT;
 INC-ENGY-LAB=9[32MEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,19;
 EMT=GAMMA'36';
 /* '36' Decay data not given */
 RSD=(95ZR,97NB);
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-LAB XSECTN-RATIO DELTA-XSECTN-RATIO
 (MEV) (NODIM) (NODIM)
 9.869E+00  6.560E-01  +-2.908E-01
 1.053E+01  7.878E-01  +-NEGLIGIBLE
 1.088E+01  8.482E-01  +-2.047E-01
 1.166E+01  8.422E-01  +-2.752E-01
 1.217E+01  7.869E-01  +-1.810E-01
 1.290E+01  8.240E-01  +-NEGLIGIBLE
 1.313E+01  7.150E-01  +-NEGLIGIBLE
 1.340E+01  8.190E-01  +-NEGLIGIBLE
 1.395E+01  6.703E-01  +-NEGLIGIBLE
 1.396E+01  8.544E-01  +-NEGLIGIBLE
 1.452E+01  8.603E-01  +-NEGLIGIBLE
 1.499E+01  8.704E-01  +-NEGLIGIBLE
 1.513E+01  9.254E-01  +-NEGLIGIBLE
 1.572E+01  8.760E-01  +-NEGLIGIBLE
 1.676E+01  7.614E-01  +-NEGLIGIBLE
 1.762E+01  5.241E-01  +-NEGLIGIBLE
 1.941E+01  7.956E-01  +-NEGLIGIBLE
 1.992E+01  7.567E-01  +-NEGLIGIBLE
 2.108E+01  8.642E-01  +-NEGLIGIBLE
 2.172E+01  9.173E-01  +-NEGLIGIBLE
 2.252E+01  9.904E-01  +-NEGLIGIBLE
 2.385E+01  8.338E-01  +-NEGLIGIBLE
 2.564E+01  5.927E-01  +-NEGLIGIBLE
 2.620E+01  7.608E-01  +-NEGLIGIBLE
 2.712E+01  7.005E-01  +-NEGLIGIBLE
 2.771E+01  7.147E-01  +-NEGLIGIBLE
 2.916E+01  7.368E-01  +-NEGLIGIBLE
 3.209E+01  8.628E-01  +-NEGLIGIBLE
 \END;
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