Exactly Soluble Spin-Glass Model

J. M. Luttinger
Phys. Rev. Lett. 37, 778 – Published 20 September 1976
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Abstract

An exactly soluble model for a spin-glass phase transition is presented. It is essentially a mean-field theory; but instead of "bond" randomness of the exchange interaction (as used by other authors), a "site" randomness is assumed. This enables one to calculate the "quenched" free energy without any uncertain mathematical procedures. Typical results are given for a variety of interesting cases.

  • Received 21 June 1976

DOI:https://doi.org/10.1103/PhysRevLett.37.778

©1976 American Physical Society

Authors & Affiliations

J. M. Luttinger*

  • The Rockefeller University, New York, New York 10021

  • *Permanent address: Department of Physics, Columbia University, New York, N. Y. 10027. This research was supported in part by the National Science Foundation.

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Vol. 37, Iss. 12 — 20 September 1976

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