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14
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0036256421
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H. Sakai, M. Kato, K. Yoshimura, and K. Kosuge, J. Phys. Soc. Jpn.71, 422 (2002).
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(2002)
J. Phys. Soc. Jpn.
, vol.71
, pp. 422
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Sakai, H.1
Kato, M.2
Yoshimura, K.3
Kosuge, K.4
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19
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0031118557
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S. Ya Istomin, O G. D’yachenko, E V. Antipov, and G. Svensson, Mater. Res. Bull.32, 421 (1997).
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(1997)
Mater. Res. Bull.
, vol.32
, pp. 421
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Ya Istomin, S.1
D’yachenko, O.G.2
Antipov, E.V.3
Svensson, G.4
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20
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0032131978
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S. Ya Istomin, O G. D’yachenko, E V. Antipov, G. Svensson, and B. Lundqvist, Mater. Res. Bull.33, 1251 (1998).
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(1998)
Mater. Res. Bull.
, vol.33
, pp. 1251
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Ya Istomin, S.1
D’yachenko, O.G.2
Antipov, E.V.3
Svensson, G.4
Lundqvist, B.5
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21
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85038945916
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H. Fukazawa, R. Higashinaka, O. Sakai, and Y. Maeno (unpublished)
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H. Fukazawa, R. Higashinaka, O. Sakai, and Y. Maeno (unpublished).
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22
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33646645869
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With the help of S. Shamoto (private communication) it was shown by a Rietveld analysis [(RIETAN-2000), and, of our x-ray diffraction data that the oxygen occupation and the oxygen position of the end member (formula presented) are those for a pyrochlore structure but not for an oxygen-deficient fluorite structure
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With the help of S. Shamoto (private communication) it was shown by a Rietveld analysis [(RIETAN-2000), F. Izumi and T. Ikeda, Mater. Sci. Forum321-324, 198 (2000)] of our x-ray diffraction data that the oxygen occupation and the oxygen position of the end member (formula presented) are those for a pyrochlore structure but not for an oxygen-deficient fluorite structure.
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(2000)
Mater. Sci. Forum
, vol.321-324
, pp. 198
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Izumi, F.1
Ikeda, T.2
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24
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85038885663
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We performed background subtraction for all the data by using the following formula: (formula presented) Here, (formula presented) and (formula presented) are the background magnetization, the magnetization with mass (formula presented) and the magnetization with mass (formula presented) respectively
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We performed background subtraction for all the data by using the following formula: (formula presented) Here, (formula presented) and (formula presented) are the background magnetization, the magnetization with mass (formula presented) and the magnetization with mass (formula presented) respectively.
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25
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85038966795
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Because of the limitation of the sample space in an oven of the magnetometer, it was necessary to reduce the sample weight. Thus, the high-temperature data was obtained under a high field of 7 T. We confirmed that the data between 300 and 350 K at 7 T with the oven quantitatively agree with those at 0.1 T without the oven
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Because of the limitation of the sample space in an oven of the magnetometer, it was necessary to reduce the sample weight. Thus, the high-temperature data was obtained under a high field of 7 T. We confirmed that the data between 300 and 350 K at 7 T with the oven quantitatively agree with those at 0.1 T without the oven.
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26
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85038968096
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K. Ishida and Y. Kitaoka (private communication)
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K. Ishida and Y. Kitaoka (private communication).
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27
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85038925970
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This difference may be attributable to the uncertainty in the demagnetization effect
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This difference may be attributable to the uncertainty in the demagnetization effect.
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28
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85038887190
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As clearly seen in Fig. 33, the Brillouin function for, larger than (formula presented) worsens the fits
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As clearly seen in Fig. 33, the Brillouin function for S larger than (formula presented) worsens the fits.
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30
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85038904060
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N. Tsuda, K. Nasu, A. Fujimori, and K. Siratori, (Shokabo, Tokyo, 1993) (in Japanese) 24, 45, and the references therein
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N. Tsuda, K. Nasu, A. Fujimori, and K. Siratori, Electronic Conduction in Oxides (Shokabo, Tokyo, 1993) (in Japanese) pp. 24, 45, and the references therein.
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32
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0036602670
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S. Shamoto, T. Nakano, Y. Nozue, and T. Kajitani, J. Phys. Chem. Solids63, 1047 (2002).
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(2002)
J. Phys. Chem. Solids
, vol.63
, pp. 1047
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Shamoto, S.1
Nakano, T.2
Nozue, Y.3
Kajitani, T.4
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33
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85038925925
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H. Harima (private communication)
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H. Harima (private communication)
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