/*===================================================================*/
 /* NRDF D1305 Data No.4                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,4;
 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 */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,4;
 /* 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=238U(P,FISSN);
 PHQ=A-DSTRN;
 INC-ENGY-LAB=12MEV;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,4;
 INC-ENGY-LAB=12MEV;
 TOT-ERR=[10%;
 EMT=GAMMA'15';
 /* '15' Decay data not given */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 A YLD
 (NODIM) (%)
 8.382E+01  1.030E+00
 8.716E+01  1.307E+00
 8.783E+01  1.661E+00
 9.032E+01  2.766E+00
 9.184E+01  2.690E+00
 9.271E+01  4.302E+00
 9.632E+01  4.464E+00
 9.803E+01  5.385E+00
 1.018E+02  4.751E+00
 1.043E+02  3.173E+00
 1.129E+02  8.415E-01
 1.145E+02  6.910E-01
 1.166E+02  4.537E-01
 1.307E+02  4.249E+00
 1.321E+02  5.551E+00
 1.330E+02  4.870E+00
 1.342E+02  5.240E+00
 1.381E+02  4.723E+00
 1.388E+02  3.788E+00
 1.400E+02  4.241E+00
 1.416E+02  2.962E+00
 1.428E+02  3.246E+00
 1.503E+02  1.253E+00
 \END;
 /*===================================================================*/