The photon emission probability in a micromaser changes drastically wh
en the kinetic energy of the pumping atoms is comparable to the atom-f
ield interaction energy. In this situation, the atomic center-of-mass
motion has to be treated quantum mechanically and the de Broglie wavel
ength of the atom inside the cavity is an important physical parameter
. The interplay between reflection and transmission of the atoms leads
to a new mechanism for induced emission. A photon is emitted by an ex
cited atom when the de Broglie wavelength fits resonantly into the cav
ity. These resonances lead to the process of microwave amplification v
ia z-motion-induced emission of radiation (mazer). We derive and illus
trate a general expression for the emission probability and a master e
quation for the mazer. We note that the probability for emission by an
excited thermal atom (stimulated maser emission) is very different fr
om the emission probability as given by the de Broglie resonances (ind
uced mazer emission). [S1050-2947(97)01411-X].