We consider electron scattering by hydrogen atoms in a bichromatic linearly
polarized laser field of frequencies omega and 3 omega and we discuss the
coherent control of the scattering process as a function of the relative ph
ase phi between the two components of the radiation held. The electrons are
assumed to have sufficiently high energies in order to permit the descript
ion of the scattering process in the first-order Born approximation. The sc
attered electrons, embedded in the bichromatic laser held of moderate power
, as well as the laser dressing of the hydrogen atoms in their ground state
are described by time-dependent perturbation theory. We discuss the angula
r dependence of the nonlinear differential scattering cross sections for th
e low values N = +/-2 of absorbed or emitted laser photons as a function of
the relative phase phi between the two radiation field components. We also
compare our results with those obtained from the assumption of a static po
tential describing the target atom.