159 elements only between states which differ in one of the
single-electron wave functions, in short, HeR induces only one-electron
transitions. The matrix elements 1mn and Pmn reduce to matrix elements
between the single-electron wave functions. We are interested primarily
in crystalline solids for which the band model is a good approximation.
The Bloch single-electron wave function in this model has the form: N'I
ili-';; U. r.;;) ( (1.14) ""nk r, =e nh\r, where n is the band index and
U (r) has the periodicity of the lattice. The form of the Bloch function
follows from the translational symmetry of the crystal, and the matrix
elements between Bloch states are subject to the condition of
wave-vector conservation: k'=k, for