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