Solution (source code)

= Solution

For $V=2λ\cos(2πx/a)$, only $U_{±1}=1$ are nonzero. To first order there is one gap of width $2λ$ at the first Brillouin-zone boundary $k=±π/a$; higher gaps vanish at this order. The allowed bands are the folded free-electron parabolas with that interval removed.