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Matsumura, Takeshi*; Tsukakoshi, Mitsuru*; Ueda, Yoshihisa*; Higa, Nonoka*; Nakao, Akiko*; Kaneko, Koji; Kakihana, Masashi*; Hedo, Masato*; Nakama, Takao*; Onuki, Yoshichika*
Journal of the Physical Society of Japan, 91(7), p.073703_1 - 073703_5, 2022/07
Times Cited Count:2 Percentile:52.46(Physics, Multidisciplinary)Higa, Nonoka*; Ito, Takashi; Yogi, Mamoru*; Hattori, Taisuke; Sakai, Hironori; Kambe, Shinsaku; Guguchia, Z.*; Higemoto, Wataru; Nakashima, Miho*; Homma, Yoshiya*; et al.
Physical Review B, 104(4), p.045145_1 - 045145_7, 2021/07
Times Cited Count:0 Percentile:0(Materials Science, Multidisciplinary)Tokunaga, Yo; Sakai, Hironori; Kambe, Shinsaku; Hattori, Taisuke; Higa, Nonoka; Nakamine, Genki*; Kitagawa, Shunsaku*; Ishida, Kenji*; Nakamura, Ai*; Shimizu, Yusei*; et al.
Journal of the Physical Society of Japan, 88(7), p.073701_1 - 073701_4, 2019/07
Times Cited Count:51 Percentile:94.85(Physics, Multidisciplinary)We report Te-NMR studies on a newly discovered heavy fermion superconductor UTe
. Using a single crystal, we have measured the
Te-NMR Knight shift
and spin-lattice relaxation rate
for fields along the three orthorhombic crystal axes. The data confirm a moderate Ising anisotropy for both the static (
) and dynamical susceptibilities (
) in the paramagnetic state above about 20 K. Around 20 K, however, we have observed a sudden loss of NMR spin-echo signal due to sudden enhancement of the NMR spin-spin relaxation rate
, when the field is applied along the easy axis of magnetization (=
axis). This behavior suggests the development of longitudinal magnetic fluctuations along the
axis at very low frequencies below 20 K.
Tokunaga, Yo; Orlova, A.*; Bruyant, N.*; Aoki, Dai*; Mayaffre, H.*; Krmer, S.*; Julien, M.-H.*; Berthier, C.*; Horvati
, M.*; Higa, Nonoka; et al.
Physical Review B, 99(8), p.085142_1 - 085142_5, 2019/02
Times Cited Count:5 Percentile:32.59(Materials Science, Multidisciplinary)The heavy-fermion antiferromagnet CeIn exhibits a field-induced anomaly associated with Fermi surface reconstruction at
45 T, well below the antiferromagnetic (AFM) critical field that exceeds 60 T. In order to explore the origin of this anomaly, we have measured
In NMR spectra in pulsed magnetic fields up to 56 T using high-quality single crystals. To within experimental resolution, we do not detect any change in the NMR spectra that could suggest a modification in either the character of the hyperfine field or the electric field gradient at In sites through
. This strongly suggests that the 45 T anomaly cannot be simply ascribed to a field-induced change in the magnetic structure of the AFM state.
Kambe, Shinsaku; Tokunaga, Yo; Sakai, Hironori; Hattori, Taisuke; Higa, Nonoka; Matsuda, Tatsuma*; Haga, Yoshinori; Walstedt, R. E.*; Harima, Hisatomo*
Physical Review B, 97(23), p.235142_1 - 235142_10, 2018/06
Times Cited Count:18 Percentile:67.99(Materials Science, Multidisciplinary)Kambe, Shinsaku; Tokunaga, Yo; Sakai, Hironori; Hattori, Taisuke; Higa, Nonoka; Uhlirova, K.*; Custers, J.*
no journal, ,
In-NQR measurements of CePtIn
were made. We succeeded in identifying at least two of the four In sites. Temperature dependent measurement of the spin lattice relaxation time was carried out. In the superconducting state. There was a strong temperature dependence of the spin lattice relaxation time. Discuss superconducting symmetry.
Sakai, Hironori; Hattori, Taisuke; Higa, Nonoka; Tokunaga, Yo; Kambe, Shinsaku; Ronning, F.*; Zhu, J.-X.*; Suzuki, Kohei*; Oshima, Yoshiki*; Yokoyama, Makoto*
no journal, ,
We have used Nuclear Quadrupole Resonance (NQR) to probe microscopically the response of prototypical quantum critical metal CeCoIn to substitutions of small amounts of Cd or Zn for In. Such non-magnetic Cd or Zn substitutions induce a long range antiferromagnetism. In the case of Cd substitutions, approximately half of the Cd substituents induce local Ce moments in their close proximity, as observed by site-dependent longitudinal nuclear spin relaxation rates
. In the paramagnetic state, the values of
at the main peak position are similar to those in the pure CeCoIn
, while those are enhanced at the skirt position of spectrum. We will discuss about the heterogeneous electronic state realized in such a Zn substituted system and discuss about the coexistence of superconductivity with the antiferromagnetism, as well.
Sakai, Hironori; Hattori, Taisuke; Higa, Nonoka; Tokunaga, Yo; Tateiwa, Naoyuki; Yamamoto, Etsuji; Haga, Yoshinori; Kambe, Shinsaku; Reyes, A. P.*; Bauer, E. D.*; et al.
no journal, ,
-US
is a paramagnetic narrow-gap semiconductor with the energy band gap of 90 K. A characteristic feature of
-US
is the strong response of the electrical resistivity to magnetic field. On the other hand, ferromagnetism is easily induced by pressure of about 1 GPa. Consequently, it is considered to be close to a ferromagnetic instability. To elucidate microscopically this very sensitive electronic states to external fields,
S-NMR study has been performed. We will show our recent
S-NMR results and discuss the electronic states.
Higa, Nonoka; Tokunaga, Yo; Hattori, Taisuke; Sakai, Hironori; Kambe, Shinsaku
no journal, ,
no abstracts in English
Sakai, Hironori; Higa, Nonoka; Hattori, Taisuke; Tokunaga, Yo; Kambe, Shinsaku; Tateiwa, Naoyuki; Haga, Yoshinori; Rossa, P. F. S.*; Thompson, J. D.*; Ronning, F.*; et al.
no journal, ,
-US
is known as a narrow-gap semiconductor. The magnetoresistance in this compound is extremely large but anisotropic. To obtain microscopic view of the magnetism, we have carried on
S-NMR study. We will discuss the magnetic properties in this system to show the recent NMR results.
Kambe, Shinsaku; Tokunaga, Yo; Sakai, Hironori; Hattori, Taisuke; Higa, Nonoka; Kratochvilova, M.*; Uhlirova, K.*; Custers, J.*
no journal, ,
no abstracts in English
Sakai, Hironori; Higa, Nonoka; Hattori, Taisuke; Tokunaga, Yo; Haga, Yoshinori; Kambe, Shinsaku; Goto, Takayuki*; Hirata, Michihiro*; Awaji, Satoshi*; Sasaki, Takahiko*
no journal, ,
We have performed Si nuclear magnetic resonance (NMR) experiments using single crystal of strongly correlated
electrons system URu
Si
under high external field of about 24 T. The temperature dependence of NMR shift in the paramagnetic state varies with external fields. The temperature and field dependences of NMR shifts resembles those of magnetic susceptibility.
Higa, Nonoka; Tokunaga, Yo; Hattori, Taisuke; Sakai, Hironori; Kambe, Shinsaku
no journal, ,
no abstracts in English
Tokunaga, Yo; Shimizu, Yusei*; Maurya, A.*; Honda, Fuminori*; Nakamura, Ai*; Sato, Yoshiki*; Li, D.*; Homma, Yoshiya*; Aoki, Dai*; Higa, Nonoka; et al.
no journal, ,
Uranium-based compound URhS exhibits two successive phase transitions at 54 K and 18 K. The origin of the phase transition at 18 K has been known to be ferromagnetic ordering, while the origin of the transition at 54 K is still unknown. In this study, we have investigated the mechanism of the successive phase transitions in URhSn by using Sn-NMR.
Tokunaga, Yo; Sakai, Hironori; Kambe, Shinsaku; Hattori, Taisuke; Higa, Nonoka*; Nakamine, Genki*; Kitagawa, Shunsaku*; Ishida, Kenji*; Nakamura, Ai*; Shimizu, Yusei*; et al.
no journal, ,
Te NMR studies have been performed on a newly discovered heavy fermion superconductor UTe
.Using a single crystal, we have measured the
Te NMR Knight shift
and spin-lattice relaxation rate
for fields along the three orthorhombic crystal axes. The data confirm a moderate Ising anisotropy for both the static (
) and dynamical susceptibilities (
) in the paramagnetic state above about 20 K. Around 20 K, however, we have observed a sudden loss of NMR spin-echo signal due to sudden enhancement of the NMR spin-spin relaxation rate
, when the field is applied along the easy axis of magnetization (=
axis).
Tokunaga, Yo; Sakai, Hironori; Kambe, Shinsaku; Hattori, Taisuke; Higa, Nonoka*; Nakamine, Genki*; Kitagawa, Shunsaku*; Ishida, Kenji*; Nakamura, Ai*; Shimizu, Yusei*; et al.
no journal, ,
Recently, Ran et al. reported evidence for superconductivity in the uranium-based heavy fermion material UTe, exhibiting the rather high transition temperature of 1.6 K. The ground state of UTe
is paramagnetic, not ferromagnetic. However, the compound still exhibits a very large and anisotropic upper critical field H
, exceeding the Pauli limit along the three principal axes, similar to the ferromagnetic superconductors, UCoGe and URhGe. Field-induced metamagnetic transition and re-entrant superconducting behaviour have been reported under strong magnetic fields around 35 T, when a magnetic field was applied along the orthorhombic hard-magnetization b-axis. In this study, we have performed Te-NMR measurements on a newly discovered heavy fermion superconductor UTe
. Our NMR data confirm a moderate Ising anisotropy for both the static (K) and dynamical susceptibilities (1/
) in the paramagnetic state above about 20 K.