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.