Berry phase in the Brillouin zone

  • Context: Undergrad 
  • Thread starter Thread starter hokhani
  • Start date Start date
  • Tags Tags
    Brillouin Phase
Click For Summary
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.

hokhani
Messages
581
Reaction score
20
As mentioned in the literatures, the definition of the Berry phase is meaningful only for non-orthogonal states. However, in the topological insulators it is defined for quantum states of a matter which are orthogonal. How to justify this inconsistency?
 
Physics news on Phys.org
Of course, in the book “A Short Course on Topological Insulators” by János K. Asbóth et. al. chapter 2, introduces the Berry phase based on the relative phase of two non-orthogonal quantum states. Then, in chapter 3 (Eq. 14), introduces the bulk electric polarization as the Berry phase of the occupied band across the Brillouin zone. I appreciate any help.
 
If I remember correctly, you are comparing orbitals within one lattice cell for different k values. These orbitals are not orthogonal. This is not in conflict with the global many electron states being orthogonal. Let ##0< |\langle \phi_1| \phi_2\rangle| <1##. Then the two local functions ##\phi_{1/2}## are not orthogonal. But the overlap of the total function of N cells goes as ##|\langle \phi_1| \phi_2\rangle|^N \to 0## if N goes to infinity.
 
  • Like
Likes   Reactions: hokhani

Similar threads

  • · Replies 10 ·
Replies
10
Views
3K
  • · Replies 18 ·
Replies
18
Views
8K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 3 ·
Replies
3
Views
6K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 22 ·
Replies
22
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K