|
| /*===================================================================*/
/* NRDF D1411 Data No.115 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,115;
D#=D1411;
TITLE=/ Mass yield curves in low-energy proton-induced fission of
233U, 235U, 236U, 237Np, 239Pu, 242Pu, 244Pu, 241Am, and 243Am
PURPOSE=/ The aim is to study more extensively the systematic
variation of mass yield curves as a function of the (Z,N) of
the fissioning nucleus and excitation energy in order to
elucidate how strongry some basic physical quantities affect
the mass division in fission. /;
ATH=(T.OHTSUKI'1,2', Y.NAGAME'2', K.TSUKADA'1', N.SHINOHARA'2',
S.BABA'2', K.HASHIMOTO'2', I.NISHINAKA'1', K.SUEKI'1',
Y.HATSUKAWA'2', K.HATA'2', T.SEKINE'2', I.KANNO'2', H.IKEZOE'2',
H.NAKAHARA'1');
INST-ATH=(2JPNTMU'1', 2JPNJAE'2');
/* '1' Department of Chemistry */
REF=PR/C;
VLP=44(1991)1405;
/* Secondary references
- PR/C, 40(1989)2144 (Preliminary results)
- PR/C, 48(1993)1667 (Systematic analysis)
RCTS=(233U(P,FISSN), 235U(P,FISSN), 236U(P,FISSN), 239PU(P,FISSN),
242PU(P,FISSN), 244PU(P,FISSN), 241AM(P,FISSN), 243AM(P,FISSN),
237NP(P,FISSN), 233U(P,FISSN)85KR, 233U(P,FISSN)87KR,
233U(P,FISSN)88KR, 233U(P,FISSN)91SR, 233U(P,FISSN)92SR,
233U(P,FISSN)93Y, 233U(P,FISSN)95ZR, 233U(P,FISSN)97ZR,
233U(P,FISSN)99MO, 233U(P,FISSN)103RU, 233U(P,FISSN)105RH,
233U(P,FISSN)112PD, 233U(P,FISSN)113AG, 233U(P,FISSN)115CD,
233U(P,FISSN)117CD, 233U(P,FISSN)126SB, 233U(P,FISSN)127SB,
233U(P,FISSN)128SB, 233U(P,FISSN)129SB, 233U(P,FISSN)130I,
233U(P,FISSN)131I, 233U(P,FISSN)132TE, 233U(P,FISSN)133I,
233U(P,FISSN)135I, 233U(P,FISSN)136CS, 233U(P,FISSN)139BA,
233U(P,FISSN)140BA, 233U(P,FISSN)141CE, 233U(P,FISSN)142LA,
233U(P,FISSN)143CE, 233U(P,FISSN)149ND, 233U(P,FISSN)153SM,
235U(P,FISSN)85KR, 235U(P,FISSN)87KR, 235U(P,FISSN)88KR,
235U(P,FISSN)91SR, 235U(P,FISSN)92SR, 235U(P,FISSN)93Y,
235U(P,FISSN)95ZR, 235U(P,FISSN)97ZR, 235U(P,FISSN)99MO,
235U(P,FISSN)103RU, 235U(P,FISSN)105RH, 235U(P,FISSN)111AG,
235U(P,FISSN)112PD, 235U(P,FISSN)113AG, 235U(P,FISSN)115CD,
235U(P,FISSN)117CD, 235U(P,FISSN)126SB, 235U(P,FISSN)127SB,
235U(P,FISSN)128SB, 235U(P,FISSN)129SB, 235U(P,FISSN)130I,
235U(P,FISSN)131I, 235U(P,FISSN)132TE, 235U(P,FISSN)133I,
235U(P,FISSN)135I, 235U(P,FISSN)136CS, 235U(P,FISSN)139BA,
235U(P,FISSN)140BA, 235U(P,FISSN)141CE, 235U(P,FISSN)142LA,
235U(P,FISSN)143CE, 235U(P,FISSN)149ND, 235U(P,FISSN)151PM,
235U(P,FISSN)153SM, 236U(P,FISSN)85KR, 236U(P,FISSN)87KR,
236U(P,FISSN)88KR, 236U(P,FISSN)91SR, 236U(P,FISSN)92SR,
236U(P,FISSN)93Y, 236U(P,FISSN)95ZR, 236U(P,FISSN)97ZR,
236U(P,FISSN)99MO, 236U(P,FISSN)103RU, 236U(P,FISSN)105RH,
236U(P,FISSN)111AG, 236U(P,FISSN)112PD, 236U(P,FISSN)113AG,
236U(P,FISSN)115CD, 236U(P,FISSN)117CD, 236U(P,FISSN)126SB,
236U(P,FISSN)127SB, 236U(P,FISSN)128SB, 236U(P,FISSN)129SB,
236U(P,FISSN)130I, 236U(P,FISSN)131I, 236U(P,FISSN)132TE,
236U(P,FISSN)133I, 236U(P,FISSN)135I, 236U(P,FISSN)136CS,
236U(P,FISSN)139BA, 236U(P,FISSN)140BA, 236U(P,FISSN)141CE,
236U(P,FISSN)142LA, 236U(P,FISSN)143CE, 236U(P,FISSN)149ND,
236U(P,FISSN)151PM, 236U(P,FISSN)153SM, 237NP(P,FISSN)85KR,
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)97ZR, 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, 237NP(P,FISSN)127SB, 237NP(P,FISSN)128SB,
237NP(P,FISSN)129SB, 237NP(P,FISSN)130I, 237NP(P,FISSN)131I,
237NP(P,FISSN)132TE, 237NP(P,FISSN)133I, 237NP(P,FISSN)135I,
237NP(P,FISSN)136CS, 237NP(P,FISSN)139BA, 237NP(P,FISSN)140BA,
237NP(P,FISSN)141CE, 237NP(P,FISSN)142LA, 237NP(P,FISSN)143CE,
237NP(P,FISSN)149ND, 237NP(P,FISSN)151PM, 237NP(P,FISSN)153SM,
239PU(P,FISSN)85KR, 239PU(P,FISSN)87KR, 239PU(P,FISSN)88KR,
239PU(P,FISSN)91SR, 239PU(P,FISSN)92SR, 239PU(P,FISSN)93Y,
239PU(P,FISSN)95ZR, 239PU(P,FISSN)97ZR, 239PU(P,FISSN)99MO,
239PU(P,FISSN)103RU, 239PU(P,FISSN)105RH, 239PU(P,FISSN)111AG,
239PU(P,FISSN)112PD, 239PU(P,FISSN)113AG, 239PU(P,FISSN)115CD,
239PU(P,FISSN)117CD, 239PU(P,FISSN)126SB, 239PU(P,FISSN)127SB,
239PU(P,FISSN)128SB, 239PU(P,FISSN)129SB, 239PU(P,FISSN)130I,
239PU(P,FISSN)131I, 239PU(P,FISSN)132TE, 239PU(P,FISSN)133I,
239PU(P,FISSN)135I, 239PU(P,FISSN)136CS, 239PU(P,FISSN)139BA,
239PU(P,FISSN)140BA, 239PU(P,FISSN)141CE, 239PU(P,FISSN)142LA,
239PU(P,FISSN)143CE, 239PU(P,FISSN)149ND, 239PU(P,FISSN)151PM,
242PU(P,FISSN)85KR, 242PU(P,FISSN)87KR, 242PU(P,FISSN)88KR,
242PU(P,FISSN)91SR, 242PU(P,FISSN)92SR, 242PU(P,FISSN)93Y,
242PU(P,FISSN)95ZR, 242PU(P,FISSN)97ZR, 242PU(P,FISSN)99MO,
242PU(P,FISSN)103RU, 242PU(P,FISSN)105RH, 242PU(P,FISSN)112PD,
242PU(P,FISSN)113AG, 242PU(P,FISSN)115CD, 242PU(P,FISSN)117CD,
242PU(P,FISSN)127SB, 242PU(P,FISSN)129SB, 242PU(P,FISSN)130I,
242PU(P,FISSN)131I, 242PU(P,FISSN)132TE, 242PU(P,FISSN)133I,
242PU(P,FISSN)135I, 242PU(P,FISSN)136CS, 242PU(P,FISSN)139BA,
242PU(P,FISSN)140BA, 242PU(P,FISSN)141CE, 242PU(P,FISSN)142LA,
242PU(P,FISSN)143CE, 242PU(P,FISSN)149ND, 242PU(P,FISSN)151PM,
242PU(P,FISSN)153SM, 244PU(P,FISSN)85KR, 244PU(P,FISSN)87KR,
244PU(P,FISSN)88KR, 244PU(P,FISSN)91SR, 244PU(P,FISSN)92SR,
244PU(P,FISSN)93Y, 244PU(P,FISSN)95ZR, 244PU(P,FISSN)97ZR,
244PU(P,FISSN)99MO, 244PU(P,FISSN)103RU, 244PU(P,FISSN)105RH,
244PU(P,FISSN)111AG, 244PU(P,FISSN)112PD, 244PU(P,FISSN)113AG,
244PU(P,FISSN)115CD, 244PU(P,FISSN)117CD, 244PU(P,FISSN)126SB,
244PU(P,FISSN)127SB, 244PU(P,FISSN)128SB, 244PU(P,FISSN)129SB,
244PU(P,FISSN)130I, 244PU(P,FISSN)131I, 244PU(P,FISSN)132TE,
244PU(P,FISSN)133I, 244PU(P,FISSN)135I, 244PU(P,FISSN)139BA,
244PU(P,FISSN)140BA, 244PU(P,FISSN)141CE, 244PU(P,FISSN)142LA,
244PU(P,FISSN)143CE, 244PU(P,FISSN)149ND, 244PU(P,FISSN)151PM,
244PU(P,FISSN)153SM, 241AM(P,FISSN)85KR, 241AM(P,FISSN)87KR,
241AM(P,FISSN)88KR, 241AM(P,FISSN)91SR, 241AM(P,FISSN)92SR,
241AM(P,FISSN)93Y, 241AM(P,FISSN)95ZR, 241AM(P,FISSN)97ZR,
241AM(P,FISSN)99MO, 241AM(P,FISSN)103RU, 241AM(P,FISSN)105RH,
241AM(P,FISSN)111AG, 241AM(P,FISSN)112PD, 241AM(P,FISSN)113AG,
241AM(P,FISSN)115CD, 241AM(P,FISSN)117CD, 241AM(P,FISSN)126SB,
241AM(P,FISSN)127SB, 241AM(P,FISSN)128SB, 241AM(P,FISSN)131I,
241AM(P,FISSN)132TE, 241AM(P,FISSN)133I, 241AM(P,FISSN)135I,
241AM(P,FISSN)136CS, 241AM(P,FISSN)139BA, 241AM(P,FISSN)140BA,
241AM(P,FISSN)141CE, 241AM(P,FISSN)142LA, 241AM(P,FISSN)143CE,
241AM(P,FISSN)149ND, 241AM(P,FISSN)151PM, 241AM(P,FISSN)153SM,
243AM(P,FISSN)85KR, 243AM(P,FISSN)87KR, 243AM(P,FISSN)91SR,
243AM(P,FISSN)92SR, 243AM(P,FISSN)93Y, 243AM(P,FISSN)97ZR,
243AM(P,FISSN)99MO, 243AM(P,FISSN)103RU, 243AM(P,FISSN)105RH,
243AM(P,FISSN)112PD, 243AM(P,FISSN)113AG, 243AM(P,FISSN)115CD,
243AM(P,FISSN)127SB, 243AM(P,FISSN)129SB, 243AM(P,FISSN)131I,
243AM(P,FISSN)132TE, 243AM(P,FISSN)133I, 243AM(P,FISSN)135I,
243AM(P,FISSN)139BA, 243AM(P,FISSN)140BA, 243AM(P,FISSN)141CE,
243AM(P,FISSN)142LA, 243AM(P,FISSN)143CE, 243AM(P,FISSN)149ND,
243AM(P,FISSN)153SM);
PHQS=XSECTN;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,115;
/* 2003-11-12 : Converted, Am + On. Data converted to EXFOR E1411
and EXFOR O0590 */
/* 2010-04-01 : Altered, Nf. 006 corrected */
RTY=FISSN;
PHQ=XSECTN;
/* Additional results shown but not compiled
- Comparison with calculated values (The weighted mean mass
number of the light and heavy asymmetric peak, the FWHM of the
heavier asymmetric peak, the peak-to-valley ratio.)
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=0.1[0.3MG/CM**2;
BAC=AL'4';
/* '4' Each target was wrapped with a sheet of Al thick enough for
stopping all fission products. */
POL-TGT=0%;
ALGN-TGT=0%;
ACC=(VDGT'5',CYC'6');
INST-ACC=(2JPNJAE'5',2JPNINS'6');
BEAM-INTNSTY=1[2UA'7';
/* '7' Their uncertainties were estimated to be about 5-10%. */
POL-PRJ=0%;
COINC=NO;
ANT-COINC=NO;
DET-SYS=HPGE;
/* Experimental Method:
- Stacked target irradiation
- Beam current integrated (The beam currents were typically 1-2
micro-A.)
- Activation (The targets were bombarded for periods of 30-min to
2-hours.)
RCT=237NP(P,FISSN)88KR;
ENR=>99.0%;
INC-ENGY-LAB-RANGE=10[32MEV;
DET-PARTCL=GAMMA'343';
/* '343' Delayed gamma from 88Kr. By compiler: Half-life 2.48
hour is probably misprinting (2.84 hour in ENSDF). */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,115;
TOT-ERR=X%'344';
/* '344' The errors cited originate from the consideration of
gamma-counting statistics and the half-life fitting for the
decay of the photopeak area. */
ENGY-GAMMA=196.3KEV'345';
INTNSTY-GAMMA=0.263'345';
HALF-LIFE=2.48HOUR'345';
/* '345' Delayed gamma from 88Kr (By compiler: Half-life 2.48
hour is probably misprinting (2.84 hour in ENSDF).) */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-LAB SIGMA DELTA-SIGMA
(MEV) (MB) (MB)
9.8 1.25 +-0.18
10.2 1.16 +-0.32
10.8 1.94 +-0.48
11.2 2.63 +-0.20
11.9 3.08 +-0.38
12.6 5.40 +-0.67
12.8 4.58 +-0.69
13.2 5.48 +-0.69
13.6 7.29 +-0.40
13.7 7.23 +-0.53
14.2 8.26 +-0.62
14.4 8.44 +-0.66
14.7 7.914 +-0.90
15.0 10.25 +-1.18
15.1 13.23 +-0.29
15.5 12.49 +-0.99
16.5 10.99 +-0.50
17.5 14.62 +-0.63
18.5 18.56 +-0.90
19.5 12.65 +-0.61
20.5 15.92 +-0.64
21.6 16.52 +-0.62
22.5 18.34 +-0.74
23.6 16.79 +-0.73
24.6 19.43 +-1.39
25.5 24.12 +-1.89
26.5 16.40 +-1.79
27.5 35.65 +-1.25
28.8 16.76 +-0.59
31.7 16.34 +-1.29
\END;
/*===================================================================*/
|