Hiroaki Yasuno
Tokyo Institute of Technology
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Featured researches published by Hiroaki Yasuno.
Japanese Journal of Applied Physics | 2003
Satoshi Wada; Hiroaki Yasuno; Takuya Hoshina; Song-Min Nam; Hirofumi Kakemoto; Takaaki Tsurumi
Barium titanate (BaTiO3) crystallites with various particle sizes from 17 to 100 nm were prepared by the 2-step thermal decomposition method of barium titanyl oxalate (BaTiO(C2O4)24H2O). The crystal structure of these BaTiO3 particles was assigned to cubic m-3m by a X-ray diffraction (XRD) measurement while it was assigned to tetragonal 4mm by a Raman scattering measurement. Investigation of impurity in these particles using both TG-DTA and FT-IR measurements revealed that no impurity was detected in the BaTiO3 lattice while hydroxyl and carbonate groups were detected only on the surface. The dielectric constants of these powders were measured using suspensions by a modified powder dielectric measurement method. As a result, the dielectric constant of BaTiO3 particles with a size of around 70 nm exhibited a maximum of over 15,000. This study revealed that BaTiO3 particles with a size around 70 nm were the most desirable for capacitor application.
Key Engineering Materials | 2003
Satoshi Wada; Takuya Hoshina; Hiroaki Yasuno; Song Min Nam; Hirofumi Kakemoto; Takaaki Tsurumi
In this study, we proposed to prepare the fine BaTiO 3 particles by a new 2 step decomposition of barium titanyl oxalate (BaTiO(C2O4)2•4H2O). The 1st step is the thermal treatment of BaTiO(C 2 4)2•4H2O at 400 ̊C for 1 hour under O 2 flow for the purpose of the removal of carbon species. The 2nd ste p is the formation of the fine BaTiO3 particles by the thermal treatment at various temperatures in vacuum. As a typical case, the fine BaTiO 3 particles with a size of about 16.5 nm were obtained by the treatm ent at 600 ̊C for 0.5 hour in vacuum. The dielectric properties of these parti cles were measured below 30MHz using the impedance analyzer. This method was composed of tw o parts; (1) the dielectric measurement using the slurry of the BaTiO 3 crystallites with 1-propanol and (2) the simulation using the electrostatic field analysis of the finite element method. When t se two kinds of the values become to same, the dielectric constant of the BaTiO 3 crystallites can be determined. Using this powder dielectric measurement, the dielectric constant of the BaTiO 3 crystallites with a size of 16.5 nm was determined at almost 400.
Ferroelectrics | 2007
Takuya Hoshina; Hiroaki Yasuno; Hirofumi Kakemoto; Takaaki Tsurumi; Satoshi Wada
Impurity-free, defect-free and dense barium titanate (BaTiO 3 ) nanoparticles with various particle sizes from 22 to 500 nm were prepared using a 2-step thermal decomposition method. Powder dielectric measurement clarified that dielectric constant of BaTiO 3 particles with 58 nm exhibited a maximum around 15,000 at 20.00°C. To explain this high dielectric constant, THz-region dielectric properties of BaTiO 3 nanoparticles, especially Slater transverse optic (TO) mode frequency, were estimated using the far infrared (FIR) reflection method. As the result, it was found that the Slater TO mode of BaTiO 3 particles with 58 nm exhibited a minimum.
Key Engineering Materials | 2006
Satoshi Wada; Takuya Hoshina; Hiroaki Yasuno; Masanori Ohishi; Hirofumi Kakemoto; Takaaki Tsurumi; Masatomo Yashima
Powder dielectric measurement of barium titanate (BaTiO3) fine particles from 17 to 1,000 nm revealed a maximum dielectric constant at a certain particle size. The sizes with maximum dielectric constants were strongly dependent on preparation methods. When BaTiO3 fine particles were prepared in vacuum of 10-2 torr, a dielectric maximum of 15,000 was observed at 70 nm. On the other hand, when BaTiO3 fine particles were prepared in air, a dielectric maximum of 5,000 was observed at 140 nm. Structure refinement of BaTiO3 particles using a Rietveld method revealed that all of BaTiO3 particles were composed of two parts; (a) surface cubic layer and (b) bulk tetragonal layer. Moreover, a thickness of surface cubic layer for BaTiO3 particles prepared in vacuum was much thinner than that for BaTiO3 particles prepared in air. To explain the differences, a new model on the basis of “surface relaxation” was proposed.
MRS Proceedings | 2004
Takaaki Tsurumi; Takashi Sekine; Hirofumi Kakemoto; Takuya Hoshina; Song-Min Nam; Hiroaki Yasuno; Satoshi Wada
Dielectric permittivity (e r ) of BaTiO 3 (BTO) powders was determined by measuring e r of slurries prepared from BTO powder and propylene carbonate as dispersion medium, followed by analyzing with a finite element methods (FEM). The e r of powders depended on their characters such as tetragonality ( c / a ratio), density, particle size and specific surface area. In order to extract the effect of each character, a statistical analysis was carried out to represent the e r of powders with an empirical formula, where the c / a ratio, density and particle size were used as parameters. A fairly good agreement between observed data and those expected from the formula was obtained and the contribution of each character to the e r could be determined.
Key Engineering Materials | 2006
Takashi Sekine; Takuya Hoshina; Song Min Nam; Hiroaki Yasuno; Hirofumi Kakemoto; Satoshi Wada; Takaaki Tsurumi
Dielectric permittivity of BaTiO3 powders was determined by measuring permittivity of slurries prepared from BaTiO3 powder and propylene carbonate as dispersion medium followed by analyzing with a finite element methods (FEM). The permittivity of powders depended on their characters such as tetragonality (c/a ratio), density, particle size and specific surface area. In order to extract the effect of each character, a statistical analysis was carried out to represent the permittivity of powders with an empirical equation where the c/a ratio, density and particle size were used as parameters. A fairly good agreement between observed data and those estimated from the relation was obtained and the contribution of each character to the permittivity could be determined.
Journal of the American Ceramic Society | 2006
Takaaki Tsurumi; Takashi Sekine; Hirofumi Kakemoto; Takuya Hoshina; Song-Min Nam; Hiroaki Yasuno; Satoshi Wada
Journal of the Korean Physical Society | 2005
Satoshi Wada; Takuya Hoshina; Hiroaki Yasuno; Song-Min Nam; Hirofumi Kakemoto; Takaaki Tsurumi; Masatomo Yashima
Journal of the Korean Physical Society | 2007
Satoshi Wada; Takuya Hoshina; Kayo Takizawa; Masanori Ohishi; Hiroaki Yasuno; H. Kakemoto; Takaaki Tsurumi; Chikako Moriyoshi; Yoshihiro Kuroiwa
Archive | 2003
Takuya Hoshina; Hirobumi Kakemoto; Takaaki Tsurumi; Tomoshi Wada; Hiroaki Yasuno; 拓也 保科; 智志 和田; 弘明 安野; 博文 掛本; 敬章 鶴見