A. Sawada
Tohoku University
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Featured researches published by A. Sawada.
Physical Review Letters | 1998
A. Sawada; Z.F. Ezawa; Hideo Ohno; Yoshiji Horikoshi; Y. Ohno; S. Kishimoto; F. Matsukura; M. Yasumoto; A. Urayama
The Hall-plateau width and the activation energy were measured in the bilayer quantum Hall state at filling factor \nu=2, 1 and 2/3, by changing the total electron density and the density ratio in the two quantum wells. Their behavior are remarkably different from one to another. The \nu=1 state is found stable over all measured range of the density difference, while the \nu=2/3
Solid State Communications | 1999
K. Muraki; Tadashi Saku; Yoshiro Hirayama; Norio Kumada; A. Sawada; Z.F. Ezawa
state is stable only around the balanced point. The \nu=2 state, on the other hand, shows a phase transition between these two types of the states as the electron density is changed.
Journal of the Physical Society of Japan | 2000
Norio Kumada; A. Sawada; Z.F. Ezawa; Satoshi Nagahama; Hirofumi Azuhata; K. Muraki; Tadashi Saku; Yoshiro Hirayama
We have studied bilayer quantum Hall (QH) effects in double-quantum-well structures at various Landau-level (LL) filling factors ν. The stability of various QH states are examined by varying the density balance between the two layers. We observe a remarkable ν-dependent behavior; the interlayer charge transfer is allowed for particular values of ν, which then repeat in a characteristic sequence with a period of 4. We employ a pseudospin picture, by which the interlayer charge transfer is expressed as a rotation of the total pseudospin. The ability or inability to accommodate the charge transfer represents the degree of pseudospin polarization in the bilayer QH state.
Solid State Communications | 1997
A. Sawada; Z.F. Ezawa; Hideo Ohno; Y. Horikoshi; Osamu Sugie; S. Kishimoto; F. Matsukura; Y. Ohno; M. Yasumoto
Skyrmion excitations were measured and compared for the first time in the bilayer quantum Hall (QH) state at the Landau-level filling factor ν=2 and in the monolayer QH state at ν=1. The observed number of flipped spins, N spin , is 14 in the bilayer sample with a large tunnelling gap, and N spin =7 in the bilayer sample with a small tunnelling gap, while it is N spin =7 in the monolayer sample. The difference is interpreted to be due to the interlayer exchange interaction.By tilting the samples in the magnetic field, we measured and compared the Skyrmion excitations in the bilayer quantum Hall (QH) state at the Landau-level filling factor
Physica B-condensed Matter | 2000
M. Kasaya; H. Suzuki; D. Tazawa; Makoto Shirakawa; A. Sawada; Toyotaka Osakabe
\nu =2
Journal of the Physical Society of Japan | 1997
Akiko Ishiguro; Hidekazu Aoki; Osamu Sugie; Michiro Suzuki; A. Sawada; N. Sato; Takemi Komatsubara; Akira Ochiai; Takashi Suzuki; Kenji Suzuki; Masahiko Higuchi; Akira Hasegawa
and in the monolayer QH state at
Journal of Magnetism and Magnetic Materials | 1998
Akiko Ishiguro; A. Sawada; Michiro Suzuki; Haruhiro Hiraka; K. Yamada; Y. Endoh; Takemi Komatsubara
\nu =1
Physica B-condensed Matter | 1998
A. Sawada; Z.F. Ezawa; Hideo Ohno; Y. Horikoshi; S. Kishimoto; F. Matsukura; Y. Ohno; M. Yasumoto; A. Urayama
. The observed number of flipped spins is
Physica B-condensed Matter | 2001
Z.F. Ezawa; A. Sawada
N_s=14
Physica E-low-dimensional Systems & Nanostructures | 2000
A. Sawada; Z.F. Ezawa; Hideo Ohno; Yoshiji Horikoshi; Norio Kumada; Y. Ohno; S. Kishimoto; F. Matsukura; Satoshi Nagahama
in the bilayer system with a large tunneling gap, and