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Prog. Theor. Phys. Vol. 5 No. 2 (1950) pp. 177-186

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The Statistics of Honeycomb and Triangular Lattice. I

Kodi Husimi and Itiro Syôzi

Department of Physics, Osaka University

(Received December 1, 1949)

Abstract:

After the matrix method in crystal statistics was introduced by R. Kubo Kramers and Wannier, and others, Onsager, using the abstract algebraic method, got the exact solution in the case of plane square net. His rather complicated method was simplified by Nambu considerably. We, independenty, attained the simplification of Onsager's method and have applied to the honeycomb lattice. And the exact solution has been obtained. From this, by the so called dual transformation we can get the partition function for triangular net.
The Curie point occurs at ch 2H = 2 in the honeycomb lattice and at exp (4H) = 3 in the triangular net. These coincide with the results obtained by the dual and star-triangle transformations. The specific heat becomes logarithmically infinite but the energy itself remains continuous at this temperature. In the antiferromagnetic case, the honeycomb lattice behaves similar to the former case but the triangular net exhibits no phase change.


URL : http://ptp.ipap.jp/link?PTP/5/177/
DOI : 10.1143/PTP.5.177

[ Full Text PDF : FREE ACCESS (589K) ] Citation:


References:

  1. R. Kubo, Busseiron Kenkyu 1 (1943).
  2. H. A. Kramers and G. H. Wannier, Phys. Rev. 60 (1941), 252[APS].
    N. W. Montroll, J. Chem. Phys. 9 (1941), 706[CrossRef]; ibid. 10 (1942), 61[CrossRef].
    E. N. Lassettre and J. P. Howe, J. Chem. Phys. 9 (1941), 747[CrossRef]; ibid. 9 (1941), 801[CrossRef].
  3. L. Onsager, Phys. Rev. 65 (1944), 117[APS].
  4. G. H. Wannier, Rev. Mod. Phys. 17 (1945), 50[APS].
  5. K. Husimi, The Quantum Statistical Mechanics, (1948), 336.
  6. Y. Nambu, Prog. Theor. Phys. 5 (1950), 1[PTP].

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