A. Harada
National Institute for Materials Science
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Featured researches published by A. Harada.
Physical Review Letters | 2010
Motoi Kimata; Taichi Terashima; Nobuyuki Kurita; Hidetaka Satsukawa; A. Harada; K. Kodama; Akira Sato; Motoharu Imai; Kunihiro Kihou; Chul-Ho Lee; Hijiri Kito; H. Eisaki; Akira Iyo; Taku Saito; Hideto Fukazawa; Yoh Kohori; Hisatomo Harima; S. Uji
We report the results of the angular-dependent magnetoresistance oscillations (AMROs), which can determine the shape of bulk Fermi surfaces (FSs) in quasi-two-dimensional (Q2D) systems, in a highly hole-doped Fe-based superconductor
Journal of Physics: Conference Series | 2012
Nobuyuki Kurita; Motoi Kimata; Kouta Kodama; A. Harada; Megumi Tomita; Hiroyuki Suzuki; Takehiko Matsumoto; Keizo Murata; Shinya Uji; Taichi Terashima
{\mathrm{KFe}}_{2}{\mathrm{As}}_{2}
arXiv: Superconductivity | 2011
Nobuyuki Kurita; Motoi Kimata; Kouta Kodama; A. Harada; Megumi Tomita; Hiroyuki Suzuki; Takehiko Matsumoto; Keizo Murata; Shinya Uji; Taichi Terashima
with
Journal of Physics: Conference Series | 2009
A. Harada; K. Enomoto; Taro Yakabe; Motoi Kimata; K Hazama; Hidetaka Satsukawa; T. Terashima; Shinya Uji
{T}_{c}\ensuremath{\approx}3.7\text{ }\text{ }\mathrm{K}
Physical Review B | 2011
Kaori Hazama; Shinya Uji; Yamaguchi Takahide; Motoi Kimata; Hidetaka Satsukawa; A. Harada; Taichi Terashima; Y. Kosaka; Hiroshi Yamamoto; R. Kato
. From the AMROs, we determined the two Q2D FSs with rounded-square cross sections, correspond to 12% and 17% of the first Brillouin zone. The rounded-squared shape of the FS cross section is also confirmed by the analyses of the interlayer transport under in-plane fields. From the obtained FS shape, we infer the character of the
Physical Review B | 2009
Motoi Kimata; Yamaguchi Takahide; A. Harada; Hidetaka Satsukawa; Kaori Hazama; Taichi Terashima; Shinya Uji; Toshio Naito; Tamotsu Inabe
3d
Physical Review B | 2010
A. Harada; K. Enomoto; Taro Yakabe; Motoi Kimata; Hidetaka Satsukawa; K Hazama; Kouta Kodama; Taichi Terashima; Shinya Uji
orbitals that contribute to the FSs.
Physica B-condensed Matter | 2010
Kouta Kodama; Motoi Kimata; Yamaguchi Takahide; T. Terashima; Hidetaka Satsukawa; A. Harada; K Hazama; Shinya Uji; Kyoji Yamamoto; Kyuya Yakushi
We have performed electrical resistivity measurements of EuFe2As2 under hydrostatic pressures (P) up to 3.2 GPa and magnetic fields up to 15 T. In zero field, the superconducting (SC) ground state with a sharp transition to zero resistivity, indicative of bulk superconductivity, emerges at Tc ~ 30 K in a pressure range from 2.5 GPa to ~ 3.0 GPa. Under applied field of 15 T, the SC transition is suppressed to lower temperatures with increasing pressure, suggesting that the application of pressure reduces the upper critical field Bc2 for the P-induced superconductivity. Meanwhile, the antiferromagnetic (AF) order of the Eu2+ moments survives up to 3.2 GPa, the highest pressure in the experiments, with no significant change in the AF ordering temperature and the magnetic field effect.
Physica B-condensed Matter | 2010
Kunihiko Kodama; Motoi Kimata; Yamaguchi Takahide; T. Terashima; Hidetaka Satsukawa; A. Harada; Kaori Hazama; Shinya Uji; Kyoji Yamamoto; Kyuya Yakushi
High-pressure electrical resistivity measurements up to 3.0 GPa have been performed on EuFe2As2 single crystals with residual resistivity ratios RRR= 7 and 15. At ambient pressure, a magnetic /structural transition related to FeAs-layers is observed at T0 = 190K and 194 K for samples with RRR= 7 and 15, respectively. Application of hydrostatic pressure suppresses T0, and then induces similar superconducting behavior in the samples with different RRR values. However, the critical pressure ~2.7 GPa, where T0 → 0, for the samples with RRR= 15 is slightly but distinctly larger than ~2.5 GPa for the samples with RRR = 7.
JJAP series | 1999
K. Kojima; A. Harada; Toshiro Takabatake; Shinichi Ogura; Koichi Hiraoka
We report the size dependence of superconducting transition in mesoscopic Al disks with 1.0, 0.7, and 0.4? m in diameter performed by resistance measurements under magnetic field. All the samples show excess resistance peaks near Hc2, which are 3 ~ 6 times larger than normal state resistance Rn, whereas there are no resistance peaks at H = 0. We find that the resistance peak rapidly increases and becomes the largest at the magnetic field just below the transition of vorticity L : 0 ? 1 with no relation to the sample size. The resistance peak, which shows the presence of large energy dissipation, would be caused by characteristic vortex dynamics confined in the small geometries.