-
1
-
-
0000910817
-
-
S. Taniguchi, T. Nishikawa, Y. Yasui, Y. Kobayashi, M. Sato, T. Nishioka, M. Kontani and K. Sano: J. Phys. Soc. Jpn. 64 (1995) 2758.
-
(1995)
J. Phys. Soc. Jpn.
, vol.64
, pp. 2758
-
-
Taniguchi, S.1
Nishikawa, T.2
Yasui, Y.3
Kobayashi, Y.4
Sato, M.5
Nishioka, T.6
Kontani, M.7
Sano, K.8
-
9
-
-
0000796718
-
-
O.A. Starykh, M.E. Zhitomirsky, D.I. Khomskii, R.R.P. Singh and K. Ueda: Phys. Rev. Lett. 77 (1996) 2558.
-
(1996)
Phys. Rev. Lett.
, vol.77
, pp. 2558
-
-
Starykh, O.A.1
Zhitomirsky, M.E.2
Khomskii, D.I.3
Singh, R.R.P.4
Ueda, K.5
-
10
-
-
0000207823
-
-
M.P. Gelfand, Z. Weihong, R.R.P. Singh, J. Oitmaa and C.J. Hamer: Phys. Rev. Lett. 77 (1996) 2794.
-
(1996)
Phys. Rev. Lett.
, vol.77
, pp. 2794
-
-
Gelfand, M.P.1
Weihong, Z.2
Singh, R.R.P.3
Oitmaa, J.4
Hamer, C.J.5
-
13
-
-
0000189301
-
-
Z. Weihong, M.P. Gelfand, R.R.P. Singh, J. Oitmaa and G.J. Hamer: Phys. Rev. B 55 (1997) 11377.
-
(1997)
Phys. Rev. B
, vol.55
, pp. 11377
-
-
Weihong, Z.1
Gelfand, M.P.2
Singh, R.R.P.3
Oitmaa, J.4
Hamer, G.J.5
-
18
-
-
0031534872
-
-
K. Kodama, H. Harashina, H. Sasaki, Y. Kobayashi, M. Kasai, S. Taniguchi, Y. Yasui, M. Sato, K. Kakurai, T. Mori and M. Nishi: J. Phys. Soc. Jpn. 66 (1997) 793.
-
(1997)
J. Phys. Soc. Jpn.
, vol.66
, pp. 793
-
-
Kodama, K.1
Harashina, H.2
Sasaki, H.3
Kobayashi, Y.4
Kasai, M.5
Taniguchi, S.6
Yasui, Y.7
Sato, M.8
Kakurai, K.9
Mori, T.10
Nishi, M.11
-
19
-
-
85024440382
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The contribution of impurity spins is expressed by the Brillouin function and a spin value of 1 is obtained. For impurity spins, however, the validity of the Brillouin function beyond the linear term in the magnetic field is not clear since spin values may be different for each impurity. Therefore we follow the standard procedure to obtain the spin part.
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S. Taniguchi, T. Nishikawa, Y. Yasui, Y. Kobayashi, M. Sato, T. Nishioka, M. Kontani and K. Sano: The spin susceptibility was obtained from the raw experimental data using the magnetic field dependence of the magnetization at 4.5 and 5 K. The contribution of impurity spins is expressed by the Brillouin function and a spin value of 1 is obtained. For impurity spins, however, the validity of the Brillouin function beyond the linear term in the magnetic field is not clear since spin values may be different for each impurity. Therefore we follow the standard procedure to obtain the spin part.
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The spin susceptibility was obtained from the raw experimental data using the magnetic field dependence of the magnetization at 4.5 and 5 K.
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Taniguchi, S.1
Nishikawa, T.2
Yasui, Y.3
Kobayashi, Y.4
Sato, M.5
Nishioka, T.6
Kontani, M.7
Sano, K.8
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20
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0031314337
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S. Taniguchi, Y. Kobayashi, M. Kasai, K. Kodama and M. Sato: J. Phys. Soc. Jpn. 66 (1997) 3660.
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(1997)
J. Phys. Soc. Jpn.
, vol.66
, pp. 3660
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Taniguchi, S.1
Kobayashi, Y.2
Kasai, M.3
Kodama, K.4
Sato, M.5
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