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Prog. Theor. Phys. Vol. 20 No. 5 (1958) pp. 614-624
Bose-Einstein Lattice Gases Equivalent to the Heisenberg Model of Ferro-, Antiferro- and Ferri-Magnetism
Tohru Morita
Physics Department, Tokyo Institute of Technology, Tokyo
(Received June 30, 1958)
Abstract:
The Hamiltonian are presented which are equivalent to the Heisenberg model of ferro-, antiferro- and ferri-magnetism and which have the form of finite power series of the Bose operators.
A technique for calculations of partition function for a system with such a Hamiltonian that contains a term of infinite potential is presented and discussed in connection with the theories of a ferromagnetic spin system by Van Kranendonk and Dyson.
URL :
http://ptp.ipap.jp/link?PTP/20/614/
DOI : 10.1143/PTP.20.614
References:
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J. Van Kranendonk and J. H. Van Vleck, Rev. Mod. Phys. 30 (1958), 1[APS].
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T. Holstein and H. Primakoff, Phys. Rev. 58 (1940), 1098[APS].
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R. Kubo, Phys. Rev. 87 (1952), 568[APS].
T. Nagamiya, K. Yoshida and R. Kubo, Adv. Phys. 4 (1955), 1.
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P. W. Anderson, Phys. Rev. 86 (1952), 694[APS].
- T. Morita, Prog. Theor. Phys. 18 (1957), 462[PTP]; See also Ref. 7.
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H. Matsuda, Prog. Theor. Phys. 18 (1957), 357[PTP].
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J. Van Kranendonk, Physica 21 (1955), 749[CrossRef];
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J. Van Kranendonk, Physica 21 (1955), 749[CrossRef];
ibid. 21 (1955), 925[CrossRef].
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F. J. Dyson, Phys. Rev. 102 (1956), 1217[APS];
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F. J. Dyson, Phys. Rev. 102 (1956), 1217[APS];
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Citing Article(s) :
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Journal of the Physical Society of Japan 64 (1995) pp. 1211-1216
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A Bose Lattice Gas Equivalent to Heisenberg Model and Its QCVM Study
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Progress of Theoretical Physics Vol. 20 No. 5 (1958) pp. 728-736
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Bose-Einstein Lattice Gas Theory of Ferromagnetism
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Progress of Theoretical Physics Vol. 27 No. 3 (1962) pp. 529-570
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Theory of Dynamical Behaviors of Ferromagnetic Spins
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Progress of Theoretical Physics Vol. 92 No. 6 (1994) pp. 1081-1093
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An Approximation Scheme of the Cluster Variation Method for Quantum Lattice Gases
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Tohru Morita
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Progress of Theoretical Physics Vol. 94 No. 1 (1995) pp. 1-9
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A Lattice-Gas Model Equivalent to the t-J Model
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