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Wallerberger, M.*; Badr, S.*; Hoshino, Shintaro*; Huber, S.*; Kakizawa, Fumiya*; Koretsune, Takashi*; Nagai, Yuki; Nogaki, Kosuke*; Nomoto, Takuya*; Mori, Hitoshi*; et al.
Software X (Internet), 21, p.101266_1 - 101266_7, 2023/02
Times Cited Count:24 Percentile:91.61(Computer Science, Software Engineering)no abstracts in English
Metoki, Naoto; Aczel, A. A.*; Aoki, Dai*; Chi, S.*; Fernandez-Baca, J. A.*; Griveau, J.-C.*; Hagihara, Masato*; Hong, T.*; Haga, Yoshinori; Ikeuchi, Kazuhiko*; et al.
JPS Conference Proceedings (Internet), 30, p.011123_1 - 011123_6, 2020/03
Rare earths (4) and actinides (5
) provide variety of interesting states realized with competing interactions between the increasing number of
electrons. Since crystal field splitting of many-body
electron system is smaller than the bandwidth, (1) high resolution experiments are needed, (2) essentially no clear spectrum with well defined peaks is expected in itinerant Ce and U compounds, and (3) Np and Pu is strictly regulated. Therefore, systematic research on magnetic excitations by neutron scattering experiments of localized compounds and rare earth iso-structural reference is useful. We describe the
electron states of heavy electron compounds NpPd
Al
and actinide and rare earth based iso-structural family.
Metoki, Naoto; Aoki, Dai*; Griveau, J.-C.*; Otsuki, Junya*
Journal of the Physical Society of Japan, 89(2), p.024707_1 - 024707_6, 2020/02
Times Cited Count:3 Percentile:25.18(Physics, Multidisciplinary)The pseudo triplet ground state in the heavy-fermion superconductor NpPdAl
was concluded. The magnetic susceptibility
can be reproduced by the singlet ground state
with the main component of
and the first excited doublet
dominated by
at
,K. The magnetization curve can be explained from the effective local hamiltonian for pseudo spin
=1 with
(
) equivalent to the quadrupole operator
. The specific heat can be described with the Kondo model normalized to give the entropy R
, corresponding to the pseudo triplet state. The derived Kondo temperature
,K comparable to the level splitting
,K indicates the contribution of the excited doublet
to the possible multi-channel Kondo effect.
Kato, Junya; Miyauchi, Atsushi; Aoshima, Atsushi; Shiotsuki, Masao; Yamashita, Teruo; Nakajima, Masayoshi; Morikawa, Yo; Miura, Akihiko; Fukui, Toshiki*; Yamasaki, Akito*; et al.
no journal, ,
no abstracts in English
Kato, Junya; Miura, Akihiko; Yamashita, Teruo; Shiotsuki, Masao
no journal, ,
no abstracts in English
Yamashita, Teruo; Miura, Akihiko; Kato, Junya; Shiotsuki, Masao; Ono, Isamu*; Fukui, Toshiki*; Yamasaki, Akito*; Matsumoto, Shiro*
no journal, ,
The objective of this development is to extend vitrification melter life-time to reduce burden of the high level radioactive waste management by applying advanced technologies. The candidate concepts of the long-life melter were studied with evaluation of adopted important advanced technologies such as skull layer conditions and the commutative electrode structure. It was concluded that such technology has a potential to extend melter life as 20 years even in the preliminary studies. Based on the obtained results, after the following fiscal year, evaluation of each component, small scale melter examination, and development and evaluation of simulation tool are carried out.
Miura, Akihiko; Kato, Junya; Yamashita, Teruo; Shiotsuki, Masao; Matsumoto, Shiro*
no journal, ,
no abstracts in English
Kato, Junya; Miura, Akihiko; Shiotsuki, Masao; Yamashita, Teruo
no journal, ,
To examine long-life vitrification melter, static corrosion tests of electrode materials are conducted to measure corrosion rate. Samples taken from the tests are observed and analyzed using SEM/EDX. As a result, NCF690 and RS311 which are the nickel based alloy show the high corrosion resistance in molten glass because high dense CrO layer is observed at the glass contact surface.
Metoki, Naoto; Aoki, Dai*; Griveau, J.-C.*; Otsuki, Junya*
no journal, ,
Non-Krammers trivalent Np(5
) ion in the heavy fermion superconductor NpPd
Al
shows
=4, similar to Pr
. We determined the singlet ground state of
and the first excited doublet of
above 49 K from the quantitative analysis of the magnetic susceptibility and the magnetization curve. The
must contribute to the heavy fermion, since the singlet ground state
alone cannot, where 2-channel Kondo effect appears based on
. The low-temperature specific heat of NpPd
Al
can be explained with the superposition of the heavy fermion state and localized Schottky anomaly, where the total entropy was maintained
ln3 for pseudo-triplet state. The
-coupling scheme of AnPd
Al
can be described by the corresponding
-
coupling scheme, where Pu and Np are the hole version of Ce and Pr. The
in NpPd
Al
is stabilized with the same mechanism as in PrT
X
, both exhibit the unconventional superconductivity.