A quantization scheme for the electromagnetic field in absorbing diele
ctrics developed previously is extended to cover more complicated arra
ngements of dielectric media and to investigate various limiting cases
of the general formalism. The limiting cases include media that have
vanishing imaginary parts in their dielectric functions, because eithe
r the refractive index or the extinction coefficient vanishes. The fur
ther limit of a unit real dielectric function establishes the connecti
on of the formalism with the well-known quantized field expressions in
free space. Detailed calculations are presented for the quantization
in the system of two different absorbing dielectrics in contact at a p
lane interface and for the cavity formed in the free space between two
separated absorbing dielectrics. The forms of the field operators are
determined for both systems, the canonical commutation relations are
verified, and the spectra of the vacuum field fluctuations are calcula
ted and illustrated. The calculations are restricted throughout to fie
lds that propagate perpendicular to the dielectric interfaces.