Bosonic mean-field theory of quantum Heisenberg spin systems: Bose condensation and magnetic order

Sanjoy Sarker, C. Jayaprakash, H. R. Krishnamurthy, and Michael Ma
Phys. Rev. B 40, 5028 – Published 1 September 1989
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Abstract

We discuss the mean-field approach to the quantum Heisenberg ferromagnet and antiferromagnet on bipartite lattices using the Schwinger boson representation, with the constraints imposed on the average. The low-dimensional results of Arovas and Auerbach [Phys. Rev. B. 38, 316 (1988)] are derived simply by using a Hartree-Fock decomposition and the Peierls variational principle. We study the models below their critical temperatures in three dimensions (and at zero temperature in d=2 dimensions) by identifying magnetic ordering with Bose condensation of the Schwinger bosons. This novel interpretation enables us to compute the low-temperature (in the ordered regime) thermodynamic properties and dispersion relations, which agree with the results of spin-wave theory. We also extract critical properties that are related to those of the spherical model. A brief discussion of the limitations of the approach is also presented.

  • Received 13 February 1989

DOI:https://doi.org/10.1103/PhysRevB.40.5028

©1989 American Physical Society

Authors & Affiliations

Sanjoy Sarker

  • Department of Physics and Astronomy, University of Alabama, P.O. Box 1921, Tuscaloosa, Alabama 35486-1921

C. Jayaprakash

  • Department of Physics, The Ohio State University, Columbus, Ohio 43210-1106

H. R. Krishnamurthy

  • Department of Physics, Princeton University, P.O. Box 708, Princeton, New Jersey 08544

Michael Ma

  • Department of Physics, University of Cincinnati, Cincinnati, Ohio 45221-0011

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Vol. 40, Iss. 7 — 1 September 1989

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