Tetuo Ohoyama
University of Electro-Communications
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Featured researches published by Tetuo Ohoyama.
Journal of the Physical Society of Japan | 1961
Kō Yasukōchi; Kazuo Kanematsu; Tetuo Ohoyama
The magnetic properties of the two intermetallic compound β phase (Fe 1.67 Ge) and δ phase (FeGe 2 ), in Fe-Ge system, were investigated. The β phase has B8 2 type of crystal structure and is ferromagnetic with the Curie point 485°K, saturation magnetization at 0°K 1.59 µ B , and paramagnetic moment 3.14 µ B per iron atom. The δ phase has C16 type of crystal structure and exhibits a parasitic ferromagnetic behavior in which the Neel point, asymptotic Curie point, saturation magnetization at 0°K, and paramagnetic moment are 190°K, +90°K, 0.11 µ B , and 2.43 µ B , per iron atom respectively. Brief discussions on the magnetic structures were given.
Journal of the Physical Society of Japan | 1961
Tetuo Ohoyama
The constitution of Mn–Ge system within the range of composition 21.8∼35.7 at.% Ge was examined X-ray powder diffraction, and magnetic properties of each phase were studied. The existence of four phases–high- and low-temperature phases at about 22∼23.5 at.% Ge ( e , e 1 ), a high temperature phase around 28 at.% Ge (ζ) and a low-temperature phase at 28.6 at.% Ge (κ)–was established. The κ phase is ferrimagnetic below the Curie point 710°K, and the spontaneous magnetization is reversed at 395°K (N type). The other phases exhibit quite anomalous magnetism. The Debye diagram for ζ phase could be indexed assuming a hexagonal structure with lattice parameters a =7.18 6 A and c =13.0 8 A.
Journal of the Physical Society of Japan | 1965
Kazuo Kanematsu; Tetuo Ohoyama
Constitution of iron-germanium system is discussed based on x-ray and magnetic studies, and a new phase diagram is proposed. Fe solid solution (α) ranges up to 20.4 at.% Ge at 710°C and to 21.3 at.% Ge at 520°C. Homogeneity range of the most iron rich compound ( e above 700°C and e 1 below) are 23.8–26 at.% Ge at 710°C ( e ) and 24.2–25.8 at.% Ge at 580°C ( e 1 ). At 50 at.% Ge, ξ phase has a narrow range below 700°C. In α (b. c. c.) solid solution of iron, the saturation magnetization and Curie point decrease to 150 emu/g and 885°K respectively. Crystal structures of e and e 1 phases are Ni 3 Sn(D0 19 ) and Cu 3 Au(L1 2 ) type, and the saturation magnetization of both phases is about 150 emu/g, while the Curie points are 650°K for e and 760°K for e 1 . ζ Phase has CoSn (B35) type of structure and is paramagnetic, the moment being 2.8µ B /Fe. Magnetic interaction and magnetic structures are also discussed.
Journal of the Physical Society of Japan | 1962
Kazuo Kanematsu; Ko Yasukochi; Tetuo Ohoyama
The susceptibilities of Co 1.67 Ge and Ni 1.67 Ge are nearly independent of temperature, and the values are 4.9×10 -6 and 0.4×10 -6 emu/g respectively. From the magnetic measurement on a series of alloys of (Co, Ni) 1.67 Ge, it is concluded that these alloys are of Pauli paramagnetism. The density of states is calculated as a function of energy, and then the effective mass ratio is estimated on the basis of the free electron theory. The ratio m * / m is about 28 for cobalt rich side, and 5 for nickel rich side. Therefore the magnetism of Co 1.67 Ge and Ni 1.67 Ge may be ascribed to the Pauli paramagnetism of 3 d holes and 4 s electrons respectively. These conclusion is consistent with a theory previously proposed.
Journal of the Physical Society of Japan | 1963
Tetuo Ohoyama; Kazuo Kanematsu; Ko Yasukochi
Journal of the Physical Society of Japan | 1968
Keizo Endo; Tetuo Ohoyama; Ren'iti Kimura
Journal of the Physical Society of Japan | 1960
Kazuo Kanematsu; Ko Yasukochi; Tetuo Ohoyama
Journal of the Physical Society of Japan | 1970
Michiko Terada; Keizo Endo; Yuko Fujita; Tetuo Ohoyama; Ren'iti Kimura
Journal of the Physical Society of Japan | 1961
Ren'iti Kimura; Tetuo Ohoyama; Keizo Endo
Journal of the Physical Society of Japan | 1962
Ren'iti Kimura; Keizo Endo; Tetuo Ohoyama