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Saptiama, I.*; Kaneti, Y. V.*; Oveisi, H.*; Suzuki, Yoshitaka; Tsuchiya, Kunihiko; Takai, Kimiko*; Sakae, Takeji*; Pradhan, S.*; Hossain, M. S. A.*; Fukumitsu, Nobuyoshi*; et al.
Bulletin of the Chemical Society of Japan, 91(2), p.195 - 200, 2018/02
Times Cited Count:53 Percentile:80.41(Chemistry, Multidisciplinary)no abstracts in English
Saptiama, I.*; Kaneti, Y. V.*; Suzuki, Yumi*; Suzuki, Yoshitaka; Tsuchiya, Kunihiko; Sakae, Takeji*; Takai, Kimiko*; Fukumitsu, Nobuyoshi*; Alothman, Z. A.*; Hossain, M. S. A.*; et al.
Bulletin of the Chemical Society of Japan, 90(10), p.1174 - 1179, 2017/10
Times Cited Count:46 Percentile:75.61(Chemistry, Multidisciplinary)no abstracts in English
quasiparticle states in
Cm by in-beam
-ray spectroscopy using heavy-ion transfer reactionsIshii, Tetsuro; Makii, Hiroyuki*; Asai, Masato; Tsukada, Kazuaki; Toyoshima, Atsushi; Matsuda, Makoto; Makishima, Akiyasu*; Shigematsu, Soichiro*; Kaneko, Junichi*; Shizuma, Toshiyuki; et al.
Physical Review C, 78(5), p.054309_1 - 054309_11, 2008/11
Times Cited Count:16 Percentile:66.66(Physics, Nuclear)
-ray spectroscopy of neutron-rich nuclei in the uranium region through the heavy-ion transfer reactionIshii, Tetsuro; Makii, Hiroyuki; Asai, Masato; Koura, Hiroyuki; Shigematsu, Soichiro*; Tsukada, Kazuaki; Toyoshima, Atsushi; Matsuda, Makoto; Makishima, Akiyasu*; Shizuma, Toshiyuki; et al.
Nuclear Physics A, 805(1-4), p.257 - 259, 2008/06
no abstracts in English
-ray study of the neutron-rich nuclei of
U,
Pu, and
Cm produced by the (
O,
O) reactionIshii, Tetsuro; Shigematsu, Soichiro*; Makii, Hiroyuki; Asai, Masato; Tsukada, Kazuaki; Toyoshima, Atsushi; Matsuda, Makoto; Makishima, Akiyasu*; Shizuma, Toshiyuki; Kaneko, Junichi*; et al.
Physics of Atomic Nuclei, 70(8), p.1457 - 1461, 2007/08
Times Cited Count:12 Percentile:62.28(Physics, Nuclear)We have measured deexcitation
rays in the neutron-rich nuclei of
U,
Pu and
Cm. These nuclei were produced by the (
O,
O) two-neutron transfer reactions with a 200, 162 and 162 MeV
O beams and a
U,
Pu and
Cm targets, respectively, using the tandem accelerator at Tokai, Japan. The
rays in residual nuclei were measured by taking coincidence with scattering particles using Si
-
detectors. We have identified
rays in
U,
Pu and
Cm by selecting the kinetic energies of
O particles which correspond to the excitation energies in these nuclei below their neutron separation energies. The ground-state bands of
U,
Pu and
Cm were established up to 12
states and the
octupole band of
U was established up to 9
state. Because the deformations of these nuclei are well developed, the moments of inertia reflect the pairing gap, which is expected to be smaller, resulting in a larger moment of inertia, at the deformed shell closure. We have found that the moment of inertia of the ground-state band of
Cm
is considerably larger than that of
Cm
. This fact supports the existence of the deformed subshell closure at
in Cm isotopes. On the other hand, the moment of inertia of
Pu
was found to be smaller than that of
Pu
, which suggests that the deformed subshell closure at
weakens or disappears in Pu isotopes. These results are consistent with the prediction by a cranking model calculation.
Th and
U nuclei and implication of spherical shell closure at 
Ishii, Tetsuro; Makii, Hiroyuki; Asai, Masato; Koura, Hiroyuki; Shigematsu, Soichiro*; Tsukada, Kazuaki; Toyoshima, Atsushi; Matsuda, Makoto; Makishima, Akiyasu*; Kaneko, Junichi*; et al.
Physical Review C, 76(1), p.011303_1 - 011303_5, 2007/07
Times Cited Count:15 Percentile:68.13(Physics, Nuclear)The ground-state bands of the neutron-rich
Th and
U nuclei were established up to spin 10 and 8, respectively, by in-beam
-ray spectroscopy using the (
O,
Ne) two-proton pickup reaction with a
U and a
Pu target. Deexcitation
rays in
Th and
U were identified by selecting the kinetic energies of
Ne using Si
-
detectors. The excitation energies of the first 2
states in U and Pu isotopes have local minima at
, suggesting the possibility that nuclei with
have a spherical shell closure of
. Calculation using the Koura-Yamada single-particle potential gives an energy gap of 1.8 MeV at
for
U.
Cm
Ishii, Tetsuro; Shigematsu, Soichiro; Makii, Hiroyuki; Asai, Masato; Tsukada, Kazuaki; Toyoshima, Atsushi; Matsuda, Makoto; Makishima, Akiyasu*; Shizuma, Toshiyuki; Kaneko, Junichi*; et al.
Journal of the Physical Society of Japan, 75(4), p.043201_1 - 043201_4, 2006/04
Times Cited Count:20 Percentile:68.28(Physics, Multidisciplinary)The ground-state band of the neutron-rich transuranium nucleus
Cm was established up to spin 12 by in-beam
-ray spectroscopy using the two-neutron-transfer reaction with a
Cm target and a 162 MeV
O beam. Deexcitation
rays in
Cm were identified by selecting the kinetic energies of
O particles with Si
-
detectors. The moment of inertia of
Cm
is considerably smaller than that of
Cm
, which supports the existence of the deformed subshell closure at
in Cm isotopes.
-ray spectroscopy of
U using the (
O,
O) reactionIshii, Tetsuro; Shigematsu, Soichiro; Asai, Masato; Makishima, Akiyasu*; Matsuda, Makoto; Kaneko, Junichi*; Hossain, I.*; Ichikawa, Shinichi; Kono, Toshiyuki*; Ogawa, Masao*
Physical Review C, 72(2), p.021301_1 - 021301_5, 2005/08
Times Cited Count:21 Percentile:76.33(Physics, Nuclear)In the two-neutron-transfer reaction of a 200-MeV
O beam with a
U target, deexcitation
rays in a neutron-rich nucleus of
U were measured. The
rays in
U were identified by taking coincidence with
O, using Si
-
detectors. The kinetic energies of
O particles allowed us to select the excitation energies of
U below the neutron separation energy. The ground-state band and the
octupole band of
U were established up to 12
and 9
, respectively. The octupole-band head of
U is higher than those of
U by about a hundred keV, suggesting that a secondary maximum of octupole correlations exists at
in U isotopes.
Ishii, Tetsuro; Asai, Masato; Makishima, Akiyasu*; Hossain, I.*; Kleinheinz, P.*; Ogawa, Masao*; Matsuda, Makoto; Ichikawa, Shinichi
European Physical Journal A, 13(1-2), p.15 - 19, 2002/01
no abstracts in English
Ishii, Tetsuro; Asai, Masato; Matsuda, Makoto; Ichikawa, Shinichi; Makishima, Akiyasu*; Hossain, I.*; Kleinheinz, P.*; Ogawa, Masao*
Acta Physica Polonica B, 32(3), p.739 - 746, 2001/03
no abstracts in English
Cu and
Co and a fast
transition in
CuAsai, Masato; Ishii, Tetsuro; Makishima, Akiyasu*; Hossain, I.*; Ogawa, Masao*; Ichikawa, Shinichi
Physical Review C, 62(5), p.054313_1 - 054313_7, 2000/11
Times Cited Count:19 Percentile:68.35(Physics, Nuclear)no abstracts in English
Ni and its neighbor
CuIshii, Tetsuro; Asai, Masato*; Makishima, A.*; Hossain, I.*; Ogawa, Masao*; Hasegawa, Jun*; Matsuda, Makoto; Ichikawa, Shinichi
Physical Review Letters, 84(1), p.39 - 42, 2000/01
Times Cited Count:67 Percentile:87.59(Physics, Multidisciplinary)no abstracts in English
Ni and its neighbor
CuIshii, Tetsuro; Asai, Masato*; Makishima, Akiyasu*; Hossain, I.*; Ogawa, Masao*; Hasegawa, Jun*; Matsuda, Makoto*; Ichikawa, Shinichi
AIP Conference Proceedings 495, p.67 - 70, 1999/12
no abstracts in English
g
p
)
- isomer in
Cu and the prediction of its
decay from the shell modelIshii, Tetsuro; Asai, Masato*; Hossain, I.*; P.Kleinheinz*; Ogawa, Masao*; Makishima, Akiyasu*; Ichikawa, Shinichi; ; ; J.Blomqvist*
Physical Review Letters, 81(19), p.4100 - 4103, 1998/11
Times Cited Count:43 Percentile:82.63(Physics, Multidisciplinary)no abstracts in English
-ray spectroscopy through deep inelastic collisionsIshii, Tetsuro; ; ; Makishima, Akiyasu*; Hossain, I.*; Hayakawa, Takehito*; Kono, Toshiyuki*; Ogawa, Masao*
Nuclear Instruments and Methods in Physics Research A, 395(2), p.210 - 216, 1997/00
Times Cited Count:45 Percentile:93.12(Instruments & Instrumentation)no abstracts in English
-ray spectroscopy of more neutron-rich nuclei than the
-stability line in the U region;
Th,
U,
Pu,
CmIshii, Tetsuro; Makii, Hiroyuki; Asai, Masato; Koura, Hiroyuki; Shigematsu, Soichiro*; Tsukada, Kazuaki; Toyoshima, Atsushi; Matsuda, Makoto; Makishima, Akiyasu*; Shizuma, Toshiyuki; et al.
no journal, ,
The ground-state bands of
Th,
U,
Pu and
Cm were established by measuring deexcitation
rays. These nuclei were produced by the (
O,
O) and (
O,
Ne) two-nucleon transfer reactions with
U,
Pu and
Cm targets. The
rays in residual nuclei were identified by taking coincidence with scattering particles using high-resolution Si
-
detectors. By extending the systematics of the 2
energies into neutron-rich nuclei, we have found that the
deformed shell gap disappears at
Pu isotopes and that U and Pu isotopes have the possibility of the spherical shell closure at
.
CmIshii, Tetsuro; Makii, Hiroyuki; Asai, Masato; Tsukada, Kazuaki; Toyoshima, Atsushi; Matsuda, Makoto; Shizuma, Toshiyuki; Makishima, Akiyasu*; Tome, Hayato*; Shigematsu, Soichiro*; et al.
no journal, ,
no abstracts in English
-ray spectroscopy of the neutron-rich
Th and
U nuclei produced by the (
O,
Ne) reactionIshii, Tetsuro; Makii, Hiroyuki; Asai, Masato; Shigematsu, Soichiro*; Tsukada, Kazuaki; Toyoshima, Atsushi; Matsuda, Makoto; Makishima, Akiyasu*; Kaneko, Junichi*; Tome, Hayato; et al.
no journal, ,
no abstracts in English
-ray measurement of the neutron-rich nucleus
Cm
Ishii, Tetsuro; Shigematsu, Soichiro; Makii, Hiroyuki; Asai, Masato; Tsukada, Kazuaki; Toyoshima, Atsushi; Matsuda, Makoto; Makishima, Akiyasu*; Shizuma, Toshiyuki; Kaneko, Junichi*; et al.
no journal, ,
no abstracts in English