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 /* NRDF D1305 Data No.21                                             */
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 /* Bibliography                                                      */
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 \\BIB,21;
 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,21;
 /* 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)103RU/237NP(P,FISSN)97NB);
 PHQ=EXC-FUNCT;
 INC-ENGY-LAB=9[32MEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,21;
 EMT=GAMMA'38';
 /* '38' Decay data not given */
 RSD=(103RU,97NB);
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-LAB XSECTN-RATIO DELTA-XSECTN-RATIO
 (MEV) (NODIM) (NODIM)
 9.421E+00  8.487E-01  +-2.768E-01
 9.641E+00  1.027E+00  +-NEGLIGIBLE
 1.084E+01  9.643E-01  +-1.934E-01
 1.136E+01  1.009E+00  +-1.578E-01
 1.195E+01  1.096E+00  +-1.299E-01
 1.267E+01  1.068E+00  +-7.815E-02
 1.305E+01  9.200E-01  +-NEGLIGIBLE
 1.308E+01  1.068E+00  +-NEGLIGIBLE
 1.325E+01  1.123E+00  +-NEGLIGIBLE
 1.350E+01  1.185E+00  +-NEGLIGIBLE
 1.372E+01  1.309E+00  +-NEGLIGIBLE
 1.402E+01  1.245E+00  +-NEGLIGIBLE
 1.428E+01  1.076E+00  +-NEGLIGIBLE
 1.481E+01  1.189E+00  +-NEGLIGIBLE
 1.517E+01  1.135E+00  +-NEGLIGIBLE
 1.656E+01  9.140E-01  +-NEGLIGIBLE
 1.762E+01  7.866E-01  +-NEGLIGIBLE
 1.853E+01  1.051E+00  +-NEGLIGIBLE
 1.953E+01  1.046E+00  +-NEGLIGIBLE
 2.083E+01  1.103E+00  +-NEGLIGIBLE
 2.139E+01  1.159E+00  +-NEGLIGIBLE
 2.241E+01  1.233E+00  +-NEGLIGIBLE
 2.375E+01  1.167E+00  +-NEGLIGIBLE
 2.497E+01  1.082E+00  +-NEGLIGIBLE
 2.569E+01  1.210E+00  +-NEGLIGIBLE
 2.636E+01  1.179E+00  +-NEGLIGIBLE
 2.724E+01  1.094E+00  +-NEGLIGIBLE
 2.847E+01  1.163E+00  +-NEGLIGIBLE
 3.181E+01  1.042E+00  +-NEGLIGIBLE
 \END;
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