Crystal momentum is the translation quantum number of a Bloch state. Since and give the same translation character whenever belongs to the reciprocal lattice, crystal momentum is defined modulo reciprocal-lattice vectors.
A charge starting at a band minimum when the field is applied acquires the displayed crystal momentum. Its orbit is a shifted circle. For masses , the real-space coordinates are proportional to and : an elliptic oscillation plus a uniform drift. Omitting the integration constant changes the physical initial condition and reduces the maximum light-axis kinetic energy by a factor of four.
A lattice-translation-invariant interaction conserves total crystal momentum modulo a reciprocal lattice vector . On a periodic chain of sites with unit spacing, the discrete Fourier transform supplies . This Fourier orthogonality proves the selection rule directly; it permits transfer by a reciprocal lattice vector rather than requiring equality of unrestricted momenta.

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  1. Bloch state
  2. Bloch's theorem
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Crystal momentum is a concept used in solid-state physics that refers to the effective momentum of particles (such as electrons) in a crystalline solid. It arises from the periodic potential of the crystal lattice in which the particles reside. In quantum mechanics, particles exhibit wave-like properties, leading to the concept of wave vectors.