Electron-phonon interaction for adiabatic anharmonic phonons
arXiv:cond-mat/0504688 · doi:10.1088/0953-8984/17/36/005
Abstract
A model with Holstein-like electron-phonon coupling is studied in the limit of adiabatic phonons. The phonon distribution is anharmonic with two degenerate maxima. This model can be related to fermions in a correlated binary alloy and describes microscopic phase separation. We discuss the weak and strong electron-phonon coupling limit and present a qualitative phase diagram. In terms of the phononic displacements it consists of a homogeneous, an alternating, and a disordered phase. There is a first order phase transition between the homogeneous and the alternating phase, and second order phase transition between the alternating and the disordered phase. The opening of a gap inside the disordered phase is treated by a dynamical mean-field theory.
11 pages, 3 figures, revised and published version
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Cited by in corpus (5)
- Instability of insulating states in optical lattices due to collective phonon excitations
- Ising instability of a Holstein phonon mode in graphene
- Path Integral of the Holstein Model with a on site potential
- Frequency splitting of intervalley phonons in graphene
- Charge-density-wave instability in the Holstein model with quartic anharmonic phonons