We consider electron scattering by hydrogen atoms in a linearly polarized l
aser field. The electrons may have sufficiently high energy in order that t
he scattering process can be treated in the first-order Born approximation.
The scattered electrons, embedded in the laser field. are described by Gor
don-Volkov waves. We assume that during the scattering, the hydrogen atoms
are in an excited state (in particular, in the 2s, 2p, or 3s state) and tha
t for moderate laser field intensities. it is sufficient to describe the in
teraction of the target atoms with the radiation field by first-order time-
dependent perturbation theory. We discuss the angular dependence of the non
linear differential scattering cross sections for low values N of emitted o
r absorbed laser photons, inspecting the contributions of the various elect
ronic and atomic terms of the matrix elements. Detailed numerical results a
re presented for one-photon absorption at low-field intensities. We also co
mpare our results with those obtained from the assumption of a static atomi
c polarizability. describing the laser dressing of the excited atomic state
s.