SUMMARY
The Berry phase is defined for non-orthogonal quantum states, yet in topological insulators, it is applicable to orthogonal states. This apparent inconsistency is addressed in "A Short Course on Topological Insulators" by János K. Asbóth et al., particularly in chapter 2, which discusses the Berry phase in relation to non-orthogonal states, and chapter 3, which connects the Berry phase to bulk electric polarization across the Brillouin zone. The discussion emphasizes that while local orbitals within a lattice cell may not be orthogonal, the global many-electron states can be orthogonal, leading to a convergence of overlap as the number of cells increases.
PREREQUISITES
- Understanding of Berry phase in quantum mechanics
- Familiarity with topological insulators
- Knowledge of the Brillouin zone concept
- Basic principles of quantum state orthogonality
NEXT STEPS
- Study the Berry phase in non-orthogonal quantum states
- Explore the properties of topological insulators in detail
- Investigate the relationship between Berry phase and bulk electric polarization
- Learn about the implications of quantum state overlap in many-electron systems
USEFUL FOR
Physicists, quantum mechanics researchers, and materials scientists interested in the properties of topological insulators and the implications of Berry phase in quantum states.