Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
for MYRRHA using a Monte Carlo techniqueIwamoto, Hiroki; Stankovskiy, A.*; Fiorito, L.*; Van den Eynde, G.*
EPJ Nuclear Sciences & Technologies (Internet), 4, p.42_1 - 42_7, 2018/11
This paper presents a nuclear data sensitivity and uncertainty analysis of the effective delayed neutron fraction
for critical and subcritical cores of the MYRRHA reactor using the continuous-energy Monte Carlo transport code MCNP. The
sensitivities are calculated by the modified
-ratio method proposed by Chiba. Comparing the
sensitivities obtained with different scaling factors
introduced by Chiba shows that a value of
is the most suitable for the uncertainty quantification of
. Using the calculated
sensitivities and the JENDL-4.0u covariance data, the
uncertainties for the critical and subcritical cores are determined to be 2.2
0.2% and 2.0
0.2%, respectively, which are dominated by delayed neutron yield of
Pu and
U.
measurement on low enriched uranyl nitrate solution with single unit cores (600
, 280T, 800
) of STACYTonoike, Kotaro; Miyoshi, Yoshinori; Kikuchi, Tsukasa*; Yamamoto, Toshihiro
Journal of Nuclear Science and Technology, 39(11), p.1227 - 1236, 2002/11
Times Cited Count:22 Percentile:77.12(Nuclear Science & Technology)Kinetic parameter
of low enriched uranyl nitrate solution was measured by the pulsed neutron source method in the STACY. This measurement was repeated systematically over several uranium concentrations from 193.7 gU/
to 432.1 gU/
. Used core tanks were two cylindrical tanks whose diameters are 600 mm and 800 mm and one slab tank which has 280 mm thickness and 700 mm width. In this report, experimental data such as solution conditions, critical solution level for each solution condition, subcritical solution levels where measurements were conducted, measured decay time constants of prompt neutron and extrapolated
values are described as well as basic principle of the pulsed neutron source method.
values were evaluated also by computation with the diffusion code CITATION in SRAC and the nuclear data library JENDL 3.2. Both experimental and computational
values show good agreement.
U,
U and
Pu by using results of in-pile measurements of effective delayed neutron fractionSakurai, Takeshi; Okajima, Shigeaki
Proceedings of International Conference on the New Frontiers of Nuclear Technology; Reactor Physics, Safety and High-Performance Computing (PHYSOR 2002) (CD-ROM), 12 Pages, 2002/10
The cross section adjustment method was applied to total delayed neutron yields of
U,
U and
Pu of the JENDL-3.2 file by using experimental results of effective delayed neutron fraction
at six cores built in two fast critical facilities of the MASURCA and FCA and a thermal critical facility of the TCA to improve these yields. The adjustment was carried out on the yields given at several incident neutron energy points in the file. Furthermore, to validate these adjusted delayed neutron yields, analyses were performed for the
experiments at ZPR fast critical facility. These adjusted yields brought a reduction of uncertainty of calculated
and an improvement in agreement of
between experiment and calculation.
U,
U and
Pu in JENDL-3.2 using benchmark experiments on effective delayed neutron fraction 
Sakurai, Takeshi; Okajima, Shigeaki
Journal of Nuclear Science and Technology, 39(1), p.19 - 30, 2002/01
Times Cited Count:6 Percentile:38.27(Nuclear Science & Technology)The cross section adjustment method was applied to total delayed neutron yields of
U,
U and
Pu of the JENDL-3.2 file by using experimental results of effective delayed neutron fraction
at six cores built in two fast critical facilities of the MASURCA and FCA and a thermal critical facility of the TCA to improve these yields. The adjustment was carried out on the yields given at several incident neutron energy points in the file. After the adjustment, the yield of
U was almost uniformly decreased by about 3% below 7 MeV. The yield of
Pu was increased by 2.6% and that of
U was decreased by 0.9% at the thermal energy point, while the change of yield was less than 0.3% at the other energy points for these nuclides. By using these adjusted yields, the uncertainty of calculated
was reduced and the agreement of
between experiment and calculation was improved.
Nakajima, Ken
Journal of Nuclear Science and Technology, 38(12), p.1120 - 1125, 2001/12
no abstracts in English

measurement and analysisKato, Yuichi*; Okajima, Shigeaki; Sakurai, Takeshi
JAERI-Data/Code 99-006, 71 Pages, 1999/03
no abstracts in English

benchmark experimentOkajima, Shigeaki; Zuhair*; Sakurai, Takeshi; H.Song*
Journal of Nuclear Science and Technology, 35(12), p.963 - 965, 1998/12
Times Cited Count:2 Percentile:23.71(Nuclear Science & Technology)no abstracts in English
Okajima, Shigeaki
Kaku Deta Nyusu (Internet), (56), p.190 - 193, 1997/00
no abstracts in English
Kaneko, Yoshihiko; Akino, Fujiyoshi;
Journal of Nuclear Science and Technology, 25(9), p.673 - 681, 1988/09
Times Cited Count:8 Percentile:64.19(Nuclear Science & Technology)no abstracts in English