Phonon-induced topological insulation
arXiv:1403.3880 · doi:10.1103/PhysRevB.89.205103
Abstract
We develop an approximate theory of phonon-induced topological insulation in Dirac materials. In the weak coupling regime, long wavelength phonons may favor topological phases in Dirac insulators with direct and narrow bandgaps. This phenomenon originates from electron-phonon matrix elements, which change qualitatively under a band inversion. A similar mechanism applies to weak Coulomb interactions and spin-independent disorder; however, the influence of these on band topology is largely independent of temperature. As applications of the theory, we evaluate the temperature-dependence of the critical thickness and the critical stoichiometric ratio for the topological transition in CdTe/HgTe quantum wells and in BiTl(SSe, respectively.
15 pages, 8 figures
References in corpus (14)
- Quantum Spin Hall Effect and Topological Phase Transition in HgTe Quantum Wells
- Intrinsic and Rashba Spin-orbit Interactions in Graphene Sheets
- Three dimensional topological invariants for time reversal invariant Hamiltonians and the three dimensional quantum spin Hall effect
- Nonlocal edge state transport in the quantum spin Hall state
- The Quantum Spin Hall Effect: Theory and Experiment
- Topological Anderson Insulator
- Realistic Time-Reversal Invariant Topological Insulators With Neutral Atoms
- Engineering Time-Reversal Invariant Topological Insulators With Ultra-Cold Atoms
- Simplified topological invariants for interacting insulators
- Topological Anderson Insulator in Three Dimensions
- Fractional topological insulators in three dimensions
- Phonon-induced topological transitions and crossovers in Dirac materials
- Thermal Instability of Protected End States in a 1-D Topological Insulator
- Disordered topological metals
Cited by in corpus (4)
- Temperature effects in the band structure of topological insulators
- Temperature-induced topological phase transitions: promoted vs. suppressed non-trivial topology
- Symmetry-protected Topological Phases at Finite Temperature
- Temperature dependence of the bulk Rashba splitting in the bismuth tellurohalides