We calculate the probability that a carrier incident on a quantum well at l
ow temperature is captured with emission of a longitudinal-optical phonon.
Our method makes use of the one-phonon self-energy of the carrier, and incl
udes some (though not all) contributions from every order in the carrier-ph
onon coupling constant. Such an approach is needed because straightforward
application of Fermi's olden rule can predict capture probabilities greater
than unity. We show that for wide quantum wells our self-energy calculatio
n can be replaced by the much simpler one of scattering by a constant, comp
lex-valued potential. Inside a quantum well the carrier's wave function is
attenuated over a distance comparable with the mean free path, so that reso
nances in the. scattering properties of the well are eventually suppressed.
[S0163-1829(99)03215-4].