Partition Functions and Stability Criteria of Topological Insulators
arXiv:1309.2155 · doi:10.1007/JHEP12(2013)101
Abstract
The non-chiral edge excitations of quantum spin Hall systems and topological insulators are described by means of their partition function. The stability of topological phases protected by time-reversal symmetry is rediscussed in this context and put in relation with the existence of discrete anomalies and the lack of modular invariance of the partition function. The characterization of stable topological insulators is extended to systems with interacting and non-Abelian edge excitations.
41 pages, 7 figures
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Cited by in corpus (16)
- Classification of topological quantum matter with symmetries
- On the coupling of Galilean-invariant field theories to curved spacetime
- Bulk-boundary correspondence in (3+1)-dimensional topological phases
- Global anomalies on the surface of fermionic symmetry-protected topological phases in (3+1) dimensions
- Symmetry-protected Topological Phases, Generalized Laughlin Argument and Orientifolds
- Conflicting Symmetries in Topologically Ordered Surface States of Three-dimensional Bosonic Symmetry Protected Topological Phases
- Topological Phases Protected By Reflection Symmetry and Cross-cap States
- fractional topological insulators in two dimensions
- Relationship between Symmetry Protected Topological Phases and Boundary Conformal Field Theories via the Entanglement Spectrum
- Global phase diagram of two-component Bose gases in antiparallel magnetic fields
- Three-dimensional Topological Insulators and Bosonization
- Coupled Wire Models of Interacting Dirac Nodal Superconductors
- Fermionic fractional quantum Hall states: A modern approach to systems with bulk-edge correspondence
- Gauging or extending bulk and boundary conformal field theories: Application to bulk and domain wall problem in topological matter and their descriptions by (mock) modular covariant
- Stability of Topological Insulators with Non-Abelian Edge Excitations
- Modular Anomalies in (2+1) and (3+1)-D Edge Theories