Mean-field cluster model for the critical behaviour of ferromagnets

Details Mean-field cluster model for the critical behaviour of ferromagnets Mean-field cluster model for the critical behaviour of ferromagnets

Nov 2000

adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2000natur.408..337c&link_type=abstract

Nature, Volume 408, Issue 6810, pp. 337-339 (2000).

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Two separate theories are often used to characterize the paramagnetic properties of ferromagnetic materials. At temperatures T well above the Curie temperature, TC (where the transition from paramagnetic to ferromagnetic behaviour occurs), classical mean-field theory yields the Curie-Weiss law for the magnetic susceptibility: χ( T) ~ 1/(T - Θ), where Θ is the Weiss constant. Close to TC, however, the standard mean-field approach breaks down so that better agreement with experimental data is provided by critical scaling theory: χ(T) ~ 1/(T - TC)γ , where γ is a scaling exponent. But there is no known model capable of predicting the measured values of γ nor its variation among different substances. Here I use a mean-field cluster model based on finite-size thermostatistics to extend the range of mean-field theory, thereby eliminating the need for a separate scaling regime. The mean-field approximation is justified by using a kinetic-energy term to maintain the microcanonical ensemble. The model reproduces the Curie-Weiss law at high temperatures, but the classical Weiss transition at TC = Θ is suppressed by finite-size effects. Instead, the fraction of clusters with a specific amount of order diverges at T C, yielding a transition that is mathematically similar to Bose-Einstein condensation. At all temperatures above T C, the model matches the measured magnetic susceptibilities of crystalline EuO, Gd, Co and Ni, thus providing a unified picture for both the critical-scaling and Curie-Weiss regimes.

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