

Author: Kennedy T.
Publisher: Springer Publishing Company
ISSN: 0022-4715
Source: Journal of Statistical Physics, Vol.91, Iss.5-6, 1998-06, pp. : 829-843
Disclaimer: Any content in publications that violate the sovereignty, the constitution or regulations of the PRC is not accepted or approved by CNPIEC.
Abstract
The Falicov–Kimball model consists of spinless electrons and classical particles (ions) on a lattice. The electrons hop between nearest neighbor sites, while the ions do not. We consider the model with equal numbers of ions and electrons and with a large on-site attractive force between ions and electrons. For densities 1/4 and 1/5, the ion configuration in the ground state had been proved to be periodic. We prove that for density 2/9 it is periodic as well. However, for densities between 1/4 and 1/5 other than 2/9 we prove that the ion configuration in the ground state is not periodic. Instead there is phase separation. For densities in (1/5, 2/9) the ground-state ion configuration is a mixture of the density 1/5 and 2/9 ground-state ion configurations. For the interval (2/9, 1/4) it is a mixture of the density 2/9 and 1/4 ground states.
Related content


Phase transition in the Falicov-Kimball model
Le Journal de Physique Colloques, Vol. 40, Iss. C5, 1979-05 ,pp. :


On Quantum Phase Transition. II. The Falicov–Kimball Model
By Messager A.
Journal of Statistical Physics, Vol. 106, Iss. 3-4, 2002-02 ,pp. :




Rigidity of Interfaces in the Falicov–Kimball Model
By Datta N. Messager A. Nachtergaele B.
Journal of Statistical Physics, Vol. 99, Iss. 1-2, 2000-04 ,pp. :


Thermodynamics of the three-dimensional Falicov-Kimball model
Journal of Physics: Conference Series , Vol. 200, Iss. 1, 2010-01 ,pp. :