/*===================================================================*/
 /* NRDF D1852 Data No.18                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,18;
 D#=D1852;
 TITLE=/Mass yield distributions in proton-induced fission of 248Cm/;
 PURPOSE=/To extend the systematic study of the mass yield distribution
          in low-energy proton-induced fission of actinides as functions
          of Z and N of the fissioning nucleus/;
 ATH=(Z.QIN'1', K.TSUKADA'1', N.SHINOHARA'1', Y.L.ZHAO'1,2',
      I.NISHINAKA'1', Y.HATSUKAWA'1', S.ICHIKAWA'1', K.HATA'1',
      Y.NAGAME'1');
 INST-ATH=(2JPNJAE'1', 2JPNTMU'2');
      /* '2' Department of Chemistry */
 REF=RCA;
 VLP=84(1999)115;
 RCTS=(248CM(P,FISSN)156SM, 248CM(P,FISSN)155SM, 248CM(P,FISSN)153SM,
       248CM(P,FISSN)151PM, 248CM(P,FISSN)149ND, 248CM(P,FISSN)147ND,
       248CM(P,FISSN)143CE, 248CM(P,FISSN)142LA, 248CM(P,FISSN)141CE,
       248CM(P,FISSN)141BA, 248CM(P,FISSN)140BA, 248CM(P,FISSN)139BA,
       248CM(P,FISSN)138CS, 248CM(P,FISSN)136CS, 248CM(P,FISSN)135I,
       248CM(P,FISSN)133I, 248CM(P,FISSN)133TE, 248CM(P,FISSN)132TE,
       248CM(P,FISSN)131I, 248CM(P,FISSN)129SB, 248CM(P,FISSN)128SN,
       248CM(P,FISSN)127SB, 248CM(P,FISSN)127SN, 248CM(P,FISSN)126SB,
       248CM(P,FISSN)117CD, 248CM(P,FISSN)115CD, 248CM(P,FISSN)113AG,
       248CM(P,FISSN)112PD, 248CM(P,FISSN)107RH, 248CM(P,FISSN)105RU,
       248CM(P,FISSN)104TC, 248CM(P,FISSN)103RU, 248CM(P,FISSN)99MO,
       248CM(P,FISSN)97ZR, 248CM(P,FISSN)95ZR, 248CM(P,FISSN)93Y,
       248CM(P,FISSN)92SR, 248CM(P,FISSN)91SR, 248CM(P,FISSN)88KR,
       248CM(P,FISSN)87KR);
 PHQS=FISSN-XSECTN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,18;
 /* 2003-11-05 : Converted, Data converted from EXFOR O0733 */
 RTY=FISSN;
 PHQ=FISSN-XSECTN;
 ENR=X%'3';
 /* '3' Isotopic composition was determined by alpha-particle
        spectrometry with a silicon surface barrier detector: 248Cm:
        96.42%, 246Cm: 3.57%, 244Cm: 0.012%, 242Cm: <0.0001% and a few
        actinide impurities of 238Pu and 241Am */
 CHM=ELM'4';
 /* '4' To remove the impurities of plutonium and some
        non-radioactive materials, especially iron and silicon which
        would disturb the electrodeposition of curium, an
        anion-exchange separation was carried out for purification. */
 PHYS-FORM=SLD;
 THK-TGT=0.05MG/CM**2'5';
 /* '5' Thickness estimated by alpha-ray spectrometry */
 BAC=AL'6';
 /* '6' Target was convered with an aluminium foil down stream to
        collect fission products. */
 THK-BAC=5.4MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNJAE;
 DELTA-INC-ENGY-LAB=XKEV'7';
 /* '7' Uncertainty of energy of proton beams was estimated to be
        about 150 to 200 keV. */
 BEAM-INTNSTY=[0.5UA'8';
 /* '8' Beam currents were monitored with a Faraday cup connected
        to a current integrator. Uncertainty of intensity of the proton
        beams was estimated to be about 6%. */
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 MONTR-RCT=/ 65CU(P,N)65ZN /;
 /* Experimental Method:
    - Beam current integrated (Beam currents were monitored with a
      Faraday cup connected to a current integrator.)
    - Activation (Proton bombardments were carried out with the
      incident energies of 20 and 13 MeV for 1 to 1.5 hour to ensure
      production of sufficient activities of fission products.)
    - Gamma ray spectrometry (Formation cross sections of each
      nuclide were determined by gamma-ray spectrometry, The nuclear
      properties of fission products used in this work are listed in
      Table 1.)
 /* Analysis:
    - Decay curve analysis
 RCT=248CM(P,FISSN)132TE;
 DET-PARTCL=GAMMA'60';
 /* '60' Delayed gamma (667.7 keV) from 132Te (Half-life=78. hour)
         is measured. Abundance of this decay mode is 1.02.667.7 keV
         gamma (emitted from 132(g)I abundance includes factor for
         genetic relationship */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,18;
 EMT=GAMMA'61';
 /* '61' Delayed Gammas */
 RSD=(132TE,65ZN);
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-LAB XSECTN DELTA-XSECTN'62'
 (MEV) (MB) (MB)
   10.5       2.1        +-0.3
   12.1       6.2        +-1.6
   13.        7.6        +-1.
   14.8       19.        +-5.
   15.9       27.        +-8.
   18.1       32.        +-6.
   20.        48.        +-13.
 \END;
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