Equation 5.63 says
q=Na2πn,(n=0,±1,±2,…) (5.63).
q=Na2πn⇒qa=2πNn; on page 223 we found that n = 0, 1, 2, … ,N – 1: Each value of n corresponds to a distinct state. To find the allowed energies we draw N horizontal lines on Figure 5.5, at heights cosqa=cos(2πn/N), and look for intersections with f(z). The point is that almost all of these lines come in pairs-two different n’s yielding the same value of cosqa:
N=1⇒n=0⇒cosqa=1. Nondegenerate.
N=2⇒n=0,1⇒cosqa=1,−1. Nondegenerate.
N=3⇒n=0,1,2⇒cosqa=1,−21,−21. The first is nondegenerate, the other two are degenerate.
N=4⇒n=0,1,2,3⇒cosqa=1,0,−1,0. Two are nondegenerate, the others are degenerate.
Evidently they are doubly degenerate (two different n’s give same cosqa) except when cosqa=±1 , i.e., at the top or bottom of a band. The Bloch factors eiqa lie at equal angles in the complex plane, starting with 1 (see figure below, drawn for the case N = 8); by symmetry, there is always one with negative imaginary part symmetrically opposite each one with positive imaginary part; these two have the same real part (cosqa). Only points which fall on the real axis have no twins.