We present an exact analytic investigation of the electron dynamics in the
field of two linearly polarized interfering copropagating laser beams of di
fferent frequencies, arbitrary intensities, and arbitrary relative polariza
tions. In one part of the paper, the laser fields are modelled by plane wav
es and in another part the fields are allowed to have one-dimensional sin(2
) pulse shapes which model focusing in the propagation direction. The gener
al situation in which the electron is injected at an angle with the common
direction of wave propagation is considered throughout. A cycle-by-cycle an
alysis of the electron motion, and its momentum and energy exchange with th
e laser fields is conducted. It is found that an electron may be accelerate
d, even from rest, to GeV energies over short distances using present-day l
aser field intensities. This leads, in principle, to energy gradients in th
e TeV m(-1) range. The trajectory calculations also show clearly that the e
lectron gets scattered away from its initial direction of motion during int
eraction with the laser fields. The transverse as well as longitudinal moti
ons may be followed exactly using our equations, and predictions could thus
be made concerning where the electron should, in principle, be ejected in
order for it to emerge with a particular energy gain.