Gap to Transition Temperature Ratio in Density Wave Ordering: a Dynamical Mean Field Study
arXiv:cond-mat/9912476 · doi:10.1103/PhysRevB.62.2424
Abstract
We use the dynamical mean-field method to determine the origin of the large ratio of the zero temperature gap to the transition temperature observed in most charge density wave materials. The method is useful because it allows an exact treatment of thermal fluctuations. We establish the relation of the dynamical mean-field results to conventional diagrammatics and thereby determine that in the physically relevant regime the origin of the large ratio is a strong inelastic scattering.
4 figures
Cited by in corpus (16)
- Exact solution of the Falicov-Kimball model with dynamical mean-field theory
- Searching for the Slater Transition in the Pyrochlore CdOsO with Infrared Spectroscopy
- Singular Effect of Disorder on Electronic Transport in Strong Coupling Electron-Phonon Systems
- Phonon Thermal Transport of URu2Si2: Broken Translational Symmetry and Strong-Coupling of the Hidden Order to the Lattice
- Phase Diagram of Half Doped Manganites
- A variational approach to the optimized phonon technique for electron-phonon problems
- Quantum phonons and the charge density wave transition temperature: a dynamical mean field study
- Benchmarking a semiclassical impurity solver for dynamical-mean-field theory: self-energies and magnetic transitions of the single-orbital Hubbard model
- Semiclassical approach to calculating the influence of local lattice fluctuations on electronic properties of metals
- Signatures of polaronic charge ordering in optical and dc conductivity using dynamical mean field theory
- Pressure effects in the triangular layered cobaltites NaxCoO2
- Infrared absorption of the charge-ordering phase: Lattice effects
- Gap ratio in anharmonic charge-density-wave systems
- The Many Electron Ground State of the Adiabatic Holstein Model in Two and Three Dimensions
- The Effect of Disorder in an Orbitally Ordered Jahn-Teller Insulator
- Collective Phase-like Mode and the Role of Lattice Distortions at TN~TC in RMn2O5 (R= Pr, Sm, Gd, Tb, Bi)