On the dynamics of polarons in the strong-coupling limit
arXiv:1612.00395 · doi:10.1142/S0129055X17500301
Abstract
The polaron model of H. Fröhlich describes an electron coupled to the quantized longitudinal optical modes of a polar crystal. In the strong-coupling limit one expects that the phonon modes may be treated classically, which leads to a coupled Schrödinger-Poisson system with memory. For the effective dynamics of the electron this amounts to a nonlinear and non-local Schrödinger equation. We use the Dirac-Frenkel variational principle to derive the Schrödinger-Poisson system from the Fröhlich model and we present new results on the accuracy of their solutions for describing the motion of Fröhlich polarons in the strong-coupling limit. Our main result extends to -polaron systems.
21 pages
References in corpus (1)
Cited by in corpus (15)
- The Dirac-Frenkel Principle for Reduced Density Matrices, and the Bogoliubov-de-Gennes Equations
- Effective Potentials Generated by Field Interaction in the Quasi-Classical Limit
- The Landau-Pekar equations: Adiabatic theorem and accuracy
- Landau-Pekar equations and quantum fluctuations for the dynamics of a strongly coupled polaron
- The Polaron at Strong Coupling
- Derivation of the Landau-Pekar equations in a many-body mean-field limit
- Mean-field Dynamics for the Nelson Model with Fermions
- A note on the Fröhlich dynamics in the strong coupling limit
- Ground State Properties in the Quasi-Classical Regime
- Optimal parabolic upper bound for the energy-momentum relation of a strongly coupled polaron
- Mean-field limits of particles in interaction with quantized radiation fields
- The effective mass problem for the Landau-Pekar equations
- Bogoliubov Dynamics and Higher-order Corrections for the Regularized Nelson Model
- Microscopic Derivation of Time-dependent Point Interactions
- Polaron catastrophe within quantum acoustics