Coherent electronic transport in periodic crystals
arXiv:2002.01990 · doi:10.1007/s00023-021-01026-3
Abstract
We consider independent electrons in a periodic crystal in their ground state, and turn on a uniform electric field at some prescribed time. We rigorously define the current per unit volume and study its properties using both linear response and adiabatic theory. Our results provide a unified framework for various phenomena such as the quantification of Hall conductivity of insulators with broken time-reversibility, the ballistic regime of electrons in metals, Bloch oscillations in the long-time response of metals, and the static conductivity of graphene. We identify explicitly the regime in which each holds.
References in corpus (14)
- Electronic transport in two dimensional graphene
- The Non-Commutative Geometry of the Quantum Hall Effect
- Triviality of Bloch and Bloch-Dirac bundles
- Effective dynamics for Bloch electrons: Peierls substitution and beyond
- Linear response theory for magnetic Schroedinger operators in disordered media
- The adiabatic theorem and linear response theory for extended quantum systems
- Optimal decay of Wannier functions in Chern and Quantum Hall insulators
- Universality of conductivity in interacting graphene
- invariants of topological insulators as geometric obstructions
- Semiclassical approximations for Hamiltonians with operator-valued symbols
- Peierls substitution for magnetic Bloch bands
- A kinetic model for the transport of electrons in a graphene layer
- An Egorov Theorem for avoided crossings of eigenvalue surfaces
- Spin Conductance and Spin Conductivity in Topological Insulators: Analysis of Kubo-like terms