Third-order spin-wave theory for the Heisenberg antiferromagnet

C. J. Hamer, Zheng Weihong, and Peter Arndt
Phys. Rev. B 46, 6276 – Published 1 September 1992
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Abstract

Spin-wave perturbation theory for the anisotropic Heisenberg antiferromagnet at zero temperature is carried to third order, using both the Dyson-Maleev and Holstein-Primakoff formalisms. Physical quantities calculated include the ground-state energy, staggered magnetization, staggered parallel susceptibility, transverse susceptibility, and energy gap. For the Holstein-Primakoff formalism, some terms diverge in the isotropic limit, but these divergences eventually cancel one another, and the final results are the same as for the Dyson-Maleev formalism. Applying these results to the square-lattice case, we find that the convergence of the spin-wave theory towards our recent estimates is further improved if we promote the spin-wave theory to third order.

  • Received 22 April 1992

DOI:https://doi.org/10.1103/PhysRevB.46.6276

©1992 American Physical Society

Authors & Affiliations

C. J. Hamer, Zheng Weihong, and Peter Arndt

  • School of Physics, The University of New South Wales, P.O. Box 1, Kensington, NSW 2033, Australia

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Vol. 46, Iss. 10 — 1 September 1992

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