Rigorous upper and lower bounds on the critical temperature in Ising models with random, quenched, broken-bond disorder
- 14 October 1977
- journal article
- Published by IOP Publishing in Journal of Physics C: Solid State Physics
- Vol. 10 (19), 3831-3849
- https://doi.org/10.1088/0022-3719/10/19/018
Abstract
Upper and lower bounds for Tc(p) are rigorously established for the Ising model with random, quenched, broken-bond disorder. Tc is the critical temperature, defined by the onset of a non-zero spontaneous magnetization, and p is the fraction of unbroken bonds. Bounds are also found for other quantities, such as the two-point correlation functions. These bounds may be applied at any temperature and any value of p with 0c and pc is the lowest value of p above which the system has a non-zero spontaneous magnetization at T=O.Keywords
This publication has 25 references indexed in Scilit:
- Bounded and inhomogeneous Ising models. III. Regularly spaced point defectsPhysical Review B, 1976
- Correlation function and transition temperature bounds for bond-disordered Ising systemsJournal of Physics C: Solid State Physics, 1975
- Critical temperature of the Heisenberg model with random bond dilutionJournal of Physics C: Solid State Physics, 1975
- Tests of strong scaling in the three-dimensional Ising modelPhysical Review B, 1975
- Renormalization of Critical Exponents by Hidden VariablesPhysical Review B, 1968
- Critical Temperatures of Anisotropic Ising Lattices. II. General Upper BoundsPhysical Review B, 1967
- Critical behaviour of a soluble model of dilute ferromagnetismProceedings of the Physical Society, 1967
- A Proof that the Free Energy of a Spin System is ExtensiveJournal of Mathematical Physics, 1964
- Ising Model and Self-Avoiding Walks on Hypercubical Lattices and "High-Density" ExpansionsPhysical Review B, 1964
- Excluded-Volume Problem and the Ising Model of FerromagnetismPhysical Review B, 1959