The band structure of absorptive dielectric photonic crystals is investigat
ed. Provided the frequency-dependent electric permeability epsilon(x, omega
) satisfies certain analyticity requirements as a function of frequency, we
show that no bandgaps exist in frequency regions where absorption takes pl
ace, i.e. where epsilon(x, omega) has a non-zero imaginary part. In this ca
se real eigenvalues of the Helmholtz operator in the Bloch-decomposed forma
lism are absent. Using a suitable analytic continuation procedure, we find
that the former change into resonances, i.e. complex numbers depending on k
, the wavevector from the first Brillouin zone, thus leading to complex ban
ds in the lower half plane. This is confirmed numerically for a simple, one
-dimensional example.