DARPE: Search Results
 /*===================================================================*/
 /* NRDF D1305 Data No.14                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,14;
 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,14;
 /* 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)87KR/237NP(P,FISSN)97NB);
 PHQ=EXC-FUNCT;
 INC-ENGY-LAB=9[32MEV;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,14;
 EMT=GAMMA'31';
 /* '31' Decay data not given */
 RSD=(87KR,97NB);
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-LAB XSECTN-RATIO DELTA-XSECTN-RATIO
 (MEV) (NODIM) (NODIM)
 1.005E+01  2.992E-01  +-1.431E-01
 1.090E+01  2.266E-01  +-7.551E-02
 1.130E+01  2.420E-01  +-5.023E-02
 1.169E+01  2.891E-01  +-7.608E-02
 1.245E+01  3.237E-01  +-NEGLIGIBLE
 1.251E+01  2.219E-01  +-4.132E-02
 1.295E+01  3.712E-01  +-NEGLIGIBLE
 1.332E+01  3.372E-01  +-6.085E-02
 1.383E+01  3.334E-01  +-6.760E-02
 1.420E+01  2.576E-01  +-NEGLIGIBLE
 1.472E+01  3.365E-01  +-6.131E-02
 1.523E+01  2.658E-01  +-7.758E-02
 1.638E+01  2.632E-01  +-5.319E-02
 1.766E+01  2.176E-01  +-3.251E-02
 1.841E+01  3.120E-01  +-6.315E-02
 1.917E+01  2.094E-01  +-3.786E-02
 2.021E+01  2.778E-01  +-5.017E-02
 2.121E+01  3.150E-01  +-6.349E-02
 2.246E+01  3.335E-01  +-5.519E-02
 2.368E+01  2.833E-01  +-5.736E-02
 2.467E+01  2.223E-01  +-5.843E-02
 2.534E+01  2.524E-01  +-NEGLIGIBLE
 2.626E+01  1.972E-01  +-NEGLIGIBLE
 2.760E+01  2.242E-01  +-NEGLIGIBLE
 2.907E+01  2.382E-01  +-NEGLIGIBLE
 3.177E+01  2.179E-01  +-3.938E-02
 \END;
 /*===================================================================*/