Extended Falicov-Kimball model: Hartree-Fock vs DMFT approach
- URL: http://arxiv.org/abs/2011.07493v1
- Date: Sun, 15 Nov 2020 10:43:55 GMT
- Title: Extended Falicov-Kimball model: Hartree-Fock vs DMFT approach
- Authors: Konrad Jerzy Kapcia (Institute of Nuclear Physics, Polish Academy of
Sciences), Romuald Lema\'nski (Institute of Low Temperature and Structure
Research, Polish Academy of Sciences), Marcin Jakub Zygmunt (Institute of
Mathematics, University of Silesia)
- Abstract summary: We study the extended Falicov-Kimball model at half-filling within the Hartree-Fock approach (HFA)
We show that the HFA description of the ground state properties of the model is equivalent to the exact DMFT solution.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: In this work, we study the extended Falicov-Kimball model at half-filling
within the Hartree-Fock approach (HFA) (for various crystal lattices) and
compare the results obtained with the rigorous ones derived within the
dynamical mean field theory (DMFT). The model describes a system, where
electrons with spin-$\downarrow$ are itinerant (with hopping amplitude $t$),
whereas those with spin-$\uparrow$ are localized. The particles interact via
on-site $U$ and intersite $V$ density-density Coulomb interactions. We show
that the HFA description of the ground state properties of the model is
equivalent to the exact DMFT solution and provides a qualitatively correct
picture also for a range of small temperatures. It does capture the
discontinuous transition between ordered phases at $U=2V$ for small
temperatures as well as correct features of the continuous order-disorder
transition. However, the HFA predicts that the discontinuous boundary ends at
the isolated-critical point (of the liquid-gas type) and it does not merge with
the continuous boundary. This approach cannot also describe properly a change
of order of the continuous transition for large $V$ as well as various
metal-insulator transitions found within the DMFT.
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