Gapless metallic charge-density-wave phase driven by strong electron correlations
arXiv:1310.4332 · doi:10.1103/PhysRevB.89.075104
Abstract
We analyze the transformation from insulator to metal induced by thermal fluctuations within the Falicov-Kimball model. Using the Dynamic Mean Field Theory (DMFT) formalism on the Bethe lattice we find rigorously the temperature dependent Density of States () at half filling in the limit of high dimensions. At zero temperature (T=0) the system is ordered to form the checkerboard pattern and the has the gap at the Fermi level , which is proportional to the interaction constant . With an increase of the evolves in various ways that depend on . For the gap persists for any (then ), so the system is always an insulator. However, if , two additional subbands develop inside the gap. They become wider with increasing and at a certain -dependent temperature they join with each other at . Since above the is positive at , we interpret as the transformation temperature from insulator to metal. It appears, that approaches the order-disorder phase transition temperature when is close to 0 or , but is substantially lower than for intermediate values of . Having calculated the temperature dependent we study thermodynamic properties of the system starting from its free energy . Then we find how the order parameter and the gap change with and we construct the phase diagram in the variables and , where we display regions of stability of four different phases: ordered insulator, ordered metal, disordered insulator and disordered metal. Finally, we use a low temperature expansion to demonstrate the existence of a nonzero DOS at a characteristic value of U on a general bipartite lattice.
19 pages, 9 figures; submitted to Physical Review B
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