## Wavefunctions of the crystal - Bloch Theorem The Hamiltonian of a semiconductor crystal has the translation symmetry with being a reciprocal lattice vector.

The Bloch theorem states that the wavefunctions have two “good” quantum numbers, the band index n and a reciprocal vector such that the wavefunctions of the crystal may be written as: where exhibits the periodicity of the crystal.

It may also be written as: Proof of Bloch’s theorem

Translation operator If R belongs to the Bravais lattice, the operator will commute with the Hamiltionian and therefore These two operators form a common set of commuting observable, we can therefore write the wavefunctions using eigenfunctions of both: Consid´erons maintenant les propri´et´es de c(R) et donc To simplify somewhat the notation, ai with i = 1, 2, 3 the basis vectors of the primitive Bravais lattice, and bi the basis vector of the reciprocal lattice. We can always define (because c(ai) is always normalized to unity: If now R is a translation of the Bravais lattice, it can be written as then, Using the orthogonality relations between the direct and reciprocal basis vectors, written as Considering the product between the vector R of the real space and the vector k of the
reciprocal space, written in the basis of the bi: and then It was in fact the result we had obtained for c(R), that was written as: setting naturally xi = ki. The wavefunctions may well be written as: that is one of the equivalent formulations of the Bloch theorem.

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