I Berry phase in the Brillouin zone

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The Berry phase is traditionally defined for non-orthogonal quantum states, yet in topological insulators, it applies to orthogonal states, raising questions about this inconsistency. The book "A Short Course on Topological Insulators" discusses the Berry phase in relation to non-orthogonal states and introduces the concept of bulk electric polarization as the Berry phase of occupied bands in the Brillouin zone. It is clarified that while local orbitals within a lattice cell may not be orthogonal, the global many-electron states can still be orthogonal. The overlap of total functions across multiple cells diminishes as the number of cells increases, supporting the use of Berry phase in this context. This discussion highlights the nuanced relationship between local and global quantum states in the framework of topological insulators.
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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?
 
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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.
 
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