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edited by M. B. Maple and F. Fisher Springer-Verlag, Berlin
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Note that the physics of the coexistence phase is not completely understood even in this classical example. See Ref. [3]; K. Machida and H. Nakanishi, Phys. Rev. B 30, 122 (1984).
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Onuki, Y.1
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Y. Ōnuki et al., J. Phys. Soc. Jpn. 61, 293 (1992); G. Oomi et al., Physica (Amsterdam) 206B-207B, 515 (1995); K. Oikawa et al., J. Phys. Soc. Jpn. 65, 3229 (1996). These references discuss the fundamental normal state properties of UGe2 both at the ambient pressure and under pressure.
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Y. Ōnuki et al., J. Phys. Soc. Jpn. 61, 293 (1992); G. Oomi et al., Physica (Amsterdam) 206B-207B, 515 (1995); K. Oikawa et al., J. Phys. Soc. Jpn. 65, 3229 (1996). These references discuss the fundamental normal state properties of UGe2 both at the ambient pressure and under pressure.
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0343755268
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to be published
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A. Huxley et al. (to be published).
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Tejima, S.1
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It is shown by T. Sugiyama and T. Ohmi [J. Phys. Soc. Jpn. 64, 7246 (1995)] that the ferromagnetic tendency stabilizes a nonunitary state, which is difficult to stabilize within the conventional weak coupling Fermi liquid framework. Thus originally a nonunitary state is quite akin to ferromagnetism in general.
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