In this paper, polaron effects in asymmetric quantum-well structures (
QW's) are investigated by using second-order perturbation theory and t
he modified Lee-Low-Pines (LLP) variational method. By applying the Gr
een's-function method, explicit analytical expressions for the electro
n extended-state wave functions and the density of states in a general
step QW's are given. Within the framework of second-order perturbatio
n theory, the ground-state polaron binding energy and effective mass i
n step and asymmetric single QW's are studied as due to the interface
optical phonons, confined bulklike LO and half-space LO phonons. The f
ull energy spectrum is included in our calculations. The effects of th
e finite electronic confinement potential and the subband nonparabolic
ity are also considered. The relative importance of the different phon
on modes is analyzed. By means of the modified LLP variational method,
the binding energy of a polaron confined to asymmetric single QW's is
also investigated. Our results show that in ordinary asymmetric QW's,
the asymmetry of the QW's has a significant influence on the polaron
effect, which has a close relationship to the interface phonon dispers
ion. When the well width and one side barrier height of asymmetric sin
gle QW's are fixed and identical with those of symmetric QW's, the pol
aron binding energy in asymmetric QW's is always smaller than that in
symmetric QW's. We have also found that it is necessary to include the
continuum energy spectrum as intermediate states in the perturbation
calculations in order to obtain the correct results; the subband nonpa
rabolicity has a small influence on the polaron effect. Comparing our
results obtained by using two different methods, good agreement is fou
nd.