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Valika, M.*; Haidamak, T.*; Cabala, A.*; Posp
il, J.*; Bastien, G.*; Sechovsk
, V.*; Prokle
ka, J.*; Yanagisawa, Tatsuya*; Opletal, P.; Sakai, Hironori; et al.
Physical Review Materials (Internet), 8(9), p.094415_1 - 094415_9, 2024/09
Times Cited Count:0 Percentile:0.00(Materials Science, Multidisciplinary)Shimamura, Kazutoshi*; Wajima, Hiroki*; Makino, Hayato*; Abe, Satoshi*; Haga, Yoshinori; Sato, Yoshiaki*; Kawae, Tatsuya*; Yoshida, Yasuo*
Japanese Journal of Applied Physics, 61(5), p.056502_1 - 056502_7, 2022/05
Times Cited Count:1 Percentile:8.10(Physics, Applied)Shimizu, Yusei*; Haga, Yoshinori; Yanagisawa, Tatsuya*; Amitsuka, Hiroshi*
Physical Review B, 93(2), p.024502_1 - 024502_8, 2016/01
Times Cited Count:8 Percentile:35.32(Materials Science, Multidisciplinary)Shimizu, Yusei*; Haga, Yoshinori; Yanagisawa, Tatsuya*; Amitsuka, Hiroshi*; Aoki, Dai*; Brison, J.-P.*; Braithwaite, D.*
JPS Conference Proceedings (Internet), 3, p.015009_1 - 015009_6, 2014/06
Shimizu, Yusei*; Haga, Yoshinori; Ikeda, Yoichi*; Yanagisawa, Tatsuya*; Amitsuka, Hiroshi*
Physical Review Letters, 109(21), p.217001_1 - 217001_5, 2012/11
Times Cited Count:18 Percentile:67.56(Physics, Multidisciplinary)Shimizu, Yusei*; Ikeda, Yoichi*; Wakabayashi, Takumi*; Haga, Yoshinori; Tenya, Kenichi*; Hidaka, Hiroyuki*; Yanagisawa, Tatsuya*; Amitsuka, Hiroshi*
Journal of the Physical Society of Japan, 80(9), p.093701_1 - 093701_4, 2011/09
Times Cited Count:8 Percentile:49.74(Physics, Multidisciplinary)Shimizu, Yusei*; Ikeda, Yoichi*; Wakabayashi, Takumi*; Tenya, Kenichi*; Haga, Yoshinori; Hidaka, Hiroyuki*; Yanagisawa, Tatsuya*; Amitsuka, Hiroshi*
Journal of the Physical Society of Japan, 80(Suppl.A), p.SA100_1 - SA100_3, 2011/07
Times Cited Count:1 Percentile:11.01(Physics, Multidisciplinary)Yanagisawa, Tatsuya*; Tateiwa, Naoyuki; Mayama, Taichi*; Saito, Hitoshi*; Hidaka, Hiroyuki*; Amitsuka, Hiroshi*; Haga, Yoshinori; Nemoto, Yuichi*; Goto, Terutaka*
Journal of the Physical Society of Japan, 80(Suppl.A), p.SA105_1 - SA105_3, 2011/07
Times Cited Count:3 Percentile:26.78(Physics, Multidisciplinary)Shimizu, Yusei*; Ikeda, Yoichi*; Wakabayashi, Takumi*; Tenya, Kenichi*; Haga, Yoshinori; Hidaka, Hiroyuki*; Yanagisawa, Tatsuya*; Amitsuka, Hiroshi*
Journal of Physics; Conference Series, 273, p.012084_1 - 012084_4, 2011/02
Times Cited Count:3 Percentile:61.86(Physics, Condensed Matter)Sakai, Hironori; Kambe, Shinsaku; Tokunaga, Yo; Fujimoto, Tatsuya; Walstedt, R. E.*; Yasuoka, Hiroshi; Aoki, Dai*; Homma, Yoshiya*; Yamamoto, Etsuji; Nakamura, Akio; et al.
Journal of Physics and Chemistry of Solids, 68(11), p.2103 - 2106, 2007/11
Times Cited Count:1 Percentile:7.31(Chemistry, Multidisciplinary)A lot of attention is currently focused on Pu-based superconductors. These systems have relatively high superconducting (SC) transition temperatures,
18 K for PuCoGa
and
9 K for PuRhGa
. Both compounds crystallize in the tetragonal HoCoGa
(115) structure, which is well known for the heavy-fermion SC systems Ce
In
(
=Co, Rh, Ir)with
2 K at most. Recently, NMR and NQR experiments have been reported for PuCoGa
by Curro et al. and for PuRhGa
by our group. In both cases, measurements of
using NQR have revealed that the Pu115 superconductors show unconventional superconductivity with an anisotropic gap. Now we have measured the more detailed data of
for NQR lines in PuRhGa
, especially focusing on the low-lying magnetic excitation in the normal state. From the viewpoint of spin-fluctuations, we will discuss the difference between PuRhGa
and PuCoGa
and between superconducting Pu115 and non-superconducting An115 series.
Tokunaga, Yo; Sakai, Hironori; Fujimoto, Tatsuya; Kambe, Shinsaku; Walstedt, R. E.*; Ikushima, Kenji*; Yasuoka, Hiroshi; Aoki, Dai*; Homma, Yoshiya*; Haga, Yoshinori; et al.
Journal of Alloys and Compounds, 444-445, p.241 - 245, 2007/10
Times Cited Count:22 Percentile:70.10(Chemistry, Physical)In this paper, we present our recent NMR works on Neptunium and Plutonium compounds. In order to elucidate the nature of the exotic multipolar ordered phase of NpO, we have initiated the first NMR measurements on this system. We have shown that direct observation of multipole order parameters is possible by means of NMR. Our NMR results provide further insight into the microscopic nature of multipole phase transitions in f-electron systems. We have also performed
Ga NMR/NQR studies on a single crystal of PuRhGa
. From the temperature dependence of the spin-lattice relaxation rate (
), we have found that PuRhGa
is an unconventional superconductor having an anisotropic superconducting (SC) gap 2
=5
. Furthermore, we have confirmed the Knight shift to be decreased below
. This gives strong evidence for spin singlet SC pairing.
Kambe, Shinsaku; Sakai, Hironori; Kato, Harukazu*; Tokunaga, Yo; Fujimoto, Tatsuya*; Walstedt, R. E.*; Ikeda, Shugo; Maehira, Takahiro*; Haga, Yoshinori; Onuki, Yoshichika
Physical Review B, 76(2), p.024411_1 - 024411_6, 2007/07
Times Cited Count:6 Percentile:30.41(Materials Science, Multidisciplinary)We report NMR studies on a single crystal of UCoGa, which has the same tetragonal HoCoGa
(115) structure as the
-wave high-
superconductor PuCoGa
. The spin-lattice relaxation rate (
) in UCoGa
issmall comparing with those of other actinide 115 compounds. This fact is consistent with a semi-metallic nature of UCoGa
suggested by de Haas-van Alphen effect measurements and band calculations. From comparison of
at crystallografically different Ga and Co sites and the static susceptibility, an existence of two bands with rather different characters is revealed.
Kambe, Shinsaku; Sakai, Hironori; Tokunaga, Yo; Fujimoto, Tatsuya*; Walstedt, R. E.*; Ikeda, Shugo; Aoki, Dai*; Homma, Yoshiya*; Haga, Yoshinori; Shiokawa, Yoshinobu*; et al.
Physical Review B, 75(14), p.140509_1 - 140509_4, 2007/04
Times Cited Count:19 Percentile:61.25(Materials Science, Multidisciplinary)We report spin-lattice relaxation time measurements in isostructural (HoCoGa type) actinide compounds withdifferent ground states (paramagnet, antiferromagnet and superconductor) using single-crystal samples. The anisotropy oflocal magnetic fluctuation due to
coupling on the actinide (magnetic) site is evaluated. In the superconductor PuRhGa
, the
type magnetic anisotropy is strong compared with non-superconducting compounds. Favorable magnetic anisotropy for
-wave superconductivity in
-electron systems is discussed.
Fujimoto, Tatsuya; Haga, Yoshinori; Sakai, Hironori; Tokunaga, Yo; Kambe, Shinsaku; Onuki, Yoshichika*
Journal of Magnetism and Magnetic Materials, 310(2, Part1), p.746 - 747, 2007/03
UPd shows the successive quadrupole orders at
K,
K and
K. The phase transition at
comes from the (1/2,0,1/2)-type quadrupole orders on quasi-cubic uranium-sublattice. On the other hand, the quadrupole states below
are still controversial; while the Polarized Neutron Diffraction suggested the triple-
structure, the Resonant X-ray Scattering assumed the canted quadrupole order. In addition, below
, an antiferromagnetic order has been suggested, but the magnetic structure and so on are not still identified. To investigate the local symmetry of the quadruple order in UPd
, we tried the nuclear quadrupole resonance, and we succeeded to find the first spin-echo signals from the UPd
probed by
Pd nuclei. In this paper, we report the nuclear properties of
Pd isotope and discuss the characteristics of the quadrupole orders emerging in each temperature phases.
Kambe, Shinsaku; Sakai, Hironori; Tokunaga, Yo; Kato, Harukazu; Fujimoto, Tatsuya; Walstedt, R. E.*; Ikeda, Shugo; Matsuda, Tatsuma; Haga, Yoshinori; Aoki, Dai*; et al.
Journal of Magnetism and Magnetic Materials, 310(2, Part1), p.176 - 181, 2007/03
performed NMR measurements in 5f-115 compounds with various ground states [UFeGa (Paramagnet), UPtGa
, NpCoGa
, NpFeGa
(Antiferromagnet) and PuRhGa
(Superconductor)], and evaluated the T-dependence of the local (actinide site) magnetic fluctuation energies (//c and c) in the paramagnetic states. An anisotropy in the magnetic fluctuations is observed in all compounds due to the strong LS coupling, in contrast to 3d-high Tc cuprates which have isotropic magnetic fluctuations at Cu sites. It is remarkable that the XY-type magnetic anisotropy is strong in PuRhGa
comparing with the non-superconducting 5f-115 compounds. The fluctuation energy in PuRhGa
is of the order of 10meV which is between of heavy fermion superconductors (1meV for
1K) and high
cuprates (102meV for
100K). The relation between the magnetic fluctuation properties and the ground states will be discussed.
Sakai, Hironori; Kambe, Shinsaku; Tokunaga, Yo; Fujimoto, Tatsuya; Walstedt, R. E.*; Yasuoka, Hiroshi; Aoki, Dai*; Homma, Yoshiya*; Yamamoto, Etsuji; Nakamura, Akio; et al.
Journal of Magnetism and Magnetic Materials, 310(2, Part1), p.e118 - e119, 2007/03
The spin-lattice relaxation rates () have been measured under zero fieldusing nuclear quadrupole resonance (NQR) linesin superconductor PuRhGa
and Pauli-paramagnet LuCoGa
. In the reference LuCoGa
with fully-occupied
shell, the
shows the constant behavior of
(sec
K)
. On the other hand, in PuRhGa
,
is much larger than in LuCoGa
and the
behavior below
30 K is seen, where its
value is 3.27
0.005 (sec
K)
. These results suggest a development of coherent Fermi liquid stateincorporated with
electronsbelow
30 K in PuRhGa
.
Sakai, Hironori; Tokunaga, Yo; Fujimoto, Tatsuya; Kambe, Shinsaku; Walstedt, R. E.; Yasuoka, Hiroshi; Aoki, Dai*; Homma, Yoshiya*; Yamamoto, Etsuji; Nakamura, Akio; et al.
Journal of the Physical Society of Japan, 75(Suppl.), p.50 - 52, 2006/08
Very recently, we have succeeded in NMR/NQR measurements for PuRhGa. PuRhGa
is a superconductor with
9 K, which is isomorphic to PuCoGa
with the higher
=18 K. We have reported that PuRhGa
is an unconventional superconductor with an anisotropic gap, through the measurement of NQR spin-lattice relaxation rate
, while PuCoGa
is also reported to be such an anisotropic superconductor. The Knight shift
and
of NMR under applied field for the normal state of PuRhGa
suggest an anisotropic feature of hyperfine and/or spin fluctuation in this system. We will outline the superconducting state and report the nature of the normal state based on the basis of
and
results. The difference between PuRhGa
and PuCoGa
will be also discussed.
Fujimoto, Tatsuya; Sakai, Hironori; Tokunaga, Yo; Kambe, Shinsaku; Walstedt, R. E.; Ikeda, Shugo; Matsuda, Tatsuma; Haga, Yoshinori; Onuki, Yoshichika
Journal of the Physical Society of Japan, 75(Suppl.), p.113 - 115, 2006/08
The low-dimensional systems exhibit wide-variety of physical properties. In the antiferromagnetic triangular lattice, for instance, resonating valence bond state is expected, furthermore, in one-dimensional (1D) systems, metal-insulator transition (Peierls transition) occurs due to charge-lattice couplings. Up to now, the study of low-dimensional systems has been mostly performed in oxides and organic compounds, but it is rare in the rare-earth and actinide intermetallics. To looking for the novel low-dimensionality in -electron systems, we focused on the UIr
B
, and NMR measurement was carried out. From Knight shift and nuclear spin-lattice relaxation rates, ferromagnetic correlations develop above 50 K, but below 50 K, the emergence of antiferromagnetic correlations was clarified along with the saturation of ferromagnetic correlations. The possible model to explain the obtained result is nesting effect on the 1D Fermi surface, and it is expected that UIr
B
will be the typical compound to investigate the physical properties of 1D
-electrons systems.
Kambe, Shinsaku; Sakai, Hironori; Tokunaga, Yo; Fujimoto, Tatsuya; Kato, Harukazu; Walstedt, R. E.; Ikeda, Shugo; Matsuda, Tatsuma; Haga, Yoshinori; Onuki, Yoshichika
Journal of the Physical Society of Japan, 75(Suppl.), p.127 - 129, 2006/08
Recently, new superconductors have been discovered in Pu-based HoCoGa(115) structure compounds: PuCoGa
(
) and PuRhGa
(
). The discovery has stimulated a lot of interest in actinide compounds. We report NMR measurements on a high-quality single crystal sample of the non-superconducting U- and Np-based 115 compounds. In order to elucidate universal magnetic properties and the origin of superconductivity in the 115 families, spin-lattice relaxation and Knight shift measurements have been performed systematically in the non-superconducting 115 compounds. Comparison of dynamical properties with the superconducting Pu115 compounds will be presented.
Fujimoto, Tatsuya; Sakai, Hironori; Tokunaga, Yo; Kambe, Shinsaku; Walstedt, R. E.; Ikeda, Shugo; Matsuda, Tatsuma; Haga, Yoshinori; Onuki, Yoshichika
Physica B; Condensed Matter, 378-380, p.997 - 998, 2006/05
Times Cited Count:0 Percentile:0.00(Physics, Condensed Matter)We report B NMR results of a single crystal UIr
B
. The measurement was performed by Fast Fourier Transformation technique, because spectral line width is extremely narrow (
10 kHz) and NMR occurs in quite limited r.f. band due to a good sample quality. From temperature variation of Knight shift and nuclear spin-lattice relaxation rate, the development of ferromagnetic correlations was clarified in the temperature range above
K. On the other hand, the magnetic dynamics was changed into another novel state below
; ferromagnetic correlations are restrained, meanwhile antiferromagnetic correlations are newly emerged. To explain this characteristic ground state, the one-dimensional
electrons state due to the unique structural lattice of UIr
B
was proposed.