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Phase Transition in the Two-Dimensional Heisenberg Ferromagnet

Vinod Mubayi*,†

Robert V. Lange

  • Laboratory of Atomic and Solid State Physics, Cornell University, Ithaca, New York 14850

  • Brandeis University, Waltham, Massachusetts 02154

  • *Work supported in part by the Advanced Research Projects Agency through the Materials Science Center, Cornell University, Report No. 958.
  • This work is based, in part, on the thesis submitted by Vinod Mubayi for the Ph.D. degree in Physics to Brandeis University in 1967.
  • Work supported in part by the National Science Foundation under contract Nos. GP-5374 and GP-7397.

Phys. Rev. 178, 882 – Published 10 February, 1969

DOI: https://doi.org/10.1103/PhysRev.178.882

Abstract

We develop a Green-function theory to describe the thermodynamic behavior of a plane square lattice with spins of magnitude one-half located at the lattice sites interacting via a nearest-neighbor Heisenberg ferromagnetic coupling. Our approximation technique involves a decoupling of the hierarchy of Green-function equations similar in some respects to that found in the random-phase approximation (RPA) but improved to include spin correlations neglected in the RPA. Such an improvement is essential for the two-dimensional problem. Our theory predicts a phase transition at the temperature given by kTc=2J, where J is the exchange parameter. As T approaches Tc from above, the static susceptibility diverges as 1(TTc). The spontaneous magnetization is zero at all nonzero temperatures, both above and below the critical point. Therefore, our theory is consistent with the existing rigorous proof of Mermin and Wagner that the spontaneous magnetization must be zero for T0, and displays the divergent susceptibility predicted by Stanley and Kaplan from an analysis of high-temperature expansions for related two-dimensional spin systems.

Comments & Replies

Comment on "Phase Transition in the Two-Dimensional Ferromagnet"

Richard P. Kenan
Phys. Rev. B 1, 3205 (1970)

References (22)

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