|
| /*===================================================================*/
/* NRDF D1411 Data No.113 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,113;
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,113;
/* 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)85KR;
ENR=>99.0%;
INC-ENGY-LAB-RANGE=10[32MEV;
DET-PARTCL=GAMMA'337';
/* '337' Delayed gamma from 85Kr (metastable state) */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,113;
TOT-ERR=X%'338';
/* '338' 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=151.2KEV'339';
INTNSTY-GAMMA=0.746'339';
HALF-LIFE=4.48HOUR'339';
/* '339' Delayed gamma from 85Kr (metastable state) */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-LAB SIGMA DELTA-SIGMA
(MEV) (MB) (MB)
9.8 0.66 +-0.09
10.2 0.65 +-0.08
10.8 1.49 +-0.22
11.2 1.46 +-0.26
11.9 2.21 +-0.34
12.6 3.17 +-0.27
12.8 3.26 +-0.66
13.2 3.94 +-1.35
13.6 4.19 +-0.33
13.7 4.26 +-0.32
14.2 5.70 +-0.27
14.4 4.51 +-0.38
14.7 5.66 +-1.63
15.0 6.11 +-1.14
15.1 5.42 +-0.94
15.5 5.57 +-1.16
16.5 6.16 +-0.14
17.5 7.13 +-1.14
18.5 8.09 +-0.20
19.5 7.77 +-1.88
20.5 6.83 +-0.98
21.6 5.59 +-0.20
22.5 5.81 +-0.25
23.6 6.56 +-0.18
24.6 7.19 +-1.65
25.5 8.25 +-0.53
26.5 9.38 +-0.83
27.5 10.58 +-0.66
28.8 10.97 +-0.50
31.7 11.41 +-0.57
\END;
/*===================================================================*/
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