This paper deals with non-Markovian behavior in atomic systems coupled to a
structured reservoir of quantum electromagnetic field modes, with particul
ar relevance to atoms interacting with the field in high-Q cavities or phot
onic band-gap materials. In cases such as the former, we show that the pseu
domode theory for single-quantum reservoir excitations can be obtained by a
pplying the Fano diagonalization method to a system in which the atomic tra
nsitions are coupled to a discrete set of (cavity) quasimodes, which in tur
n are coupled to a continuum set of (external) quasimodes with slowly varyi
ng coupling constants and continuum mode density. Each pseudomode can be id
entified with a discrete quasimode, which gives structure to the actual res
ervoir of true modes via the expressions for the equivalent atom-true mode
coupling constants. The quasimode theory enables cases of multiple excitati
on of the reservoir to now be treated via Markovian master equations for th
e atom-discrete quasimode system. Applications of the theory to one, two, a
nd many discrete quasimodes are made. For a simple photonic band-gap model,
where the reservoir structure is associated with the true mode density rat
her than the coupling constants, the single quantum excitation case appears
to be equivalent to a case with two discrete quasimodes.