Shoichi Nagata
Hokkaido University
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Featured researches published by Shoichi Nagata.
Journal of the Physical Society of Japan | 1975
Hisao Kitaguchi; Shoichi Nagata; Takashi Watanabe
The magnetic susceptibility and the specific heat of Cu(NH 3 ) 2 ·Ni(CN) 4 ·2C 6 H 6 in powder specimen has been measured between 0.2 and 20.4 K. Broad maximums are observed near 3 K in both experimental results, but the information for phase transition to the long range order can not be obtained down to 0.2 K. These results give the behaviour of low dimensional magnetic lattice for this crystal. The susceptibility data is explained as the one dimensional antiferromagnetic spin system with exchange interaction | J |=2.31 K.
Journal of the Physical Society of Japan | 1976
Hisao Kitaguchi; Shoichi Nagata; Takashi Watanabe
The magnetic susceptibility and the specific heat of Mn(NH 3 ) 2 ·Ni(CN) 4 ·2C 6 H 6 for powder specimen have been measured from 0.3 K to 20 K. The Neel temperature is found at 0.66 K. The Weiss temperature is obtained as –1.52 K with antiferromagnetic coupling. The relation between susceptibility and specific heat which is known as the Fishers relation is experimentally verified. The broad maximum of specific heat is observed near 3 K. The origin is not explained as magnetic system through the entropy analysis.
Journal of the Physical Society of Japan | 1973
Shoichi Nagata; Yoshihito Miyako; Takashi Watanabe
ESR for isolated Cu 2+ ions and exchange-coupled pairs of Cu 2+ ions in diamagnetic single crystal of Cd(NH 3 ) 2 ·Ni(CN) 4 ·2C 6 H 6 have been studied. As for the isolated ions, the spin Hamiltonian parameters, g , A and the transferred hyperfine constant due to the neighbouring nitrogen ions are determined. As for the Cu 2+ pairs, the ground state is concluded to be antiferromagnetic with the exchange parameter J of (7±1) K from the temperature dependence of their intensity.
Archive | 1974
H. Kitaguchi; Shoichi Nagata; Yoshihito Miyako; T. Watanabe
The crystal symmetry of Cu(NH3)2 · Ni(CN)4 · 2C6H6 is tetragonal and the space group is P 4/m, as shown in Fig. 1.1,2 The magnetic susceptibility was measured by the ac Hartshon bridge method at 80 Hz. The temperature range for the present experimental measurement is between 0.2 and 20.4°K. The temperature range in the specific heat measurement is between 1.2 and 20.4°K.3,4
Journal of the Physical Society of Japan | 1971
Shoichi Nagata; Tsuyoshi Maruyamauchi; Takashi Watanabe
Journal of the Physical Society of Japan | 1974
Shoichi Nagata
Journal of the Physical Society of Japan | 1977
Yoshihide Kimishima; Satoru Simizu; Shoichi Nagata; Takashi Watanabe
Journal of the Physical Society of Japan | 1985
Shoichi Nagata
Journal of the Physical Society of Japan | 1977
Yoshihide Kimishima; Satoru Simizu; Shoichi Nagata; Takashi Watanabe
Journal of the Physical Society of Japan | 1977
Yoshihide Kimishima; Satoru Simizu; Shoichi Nagata; Takashi Watanabe