We investigate electron-ion recombination in a powerful bichromatic laser f
ield of frequencies omega (L) and 3 omega (L) and consider the dependence o
f the recombination probabilities on the relative phase phi of the two held
components. During this process a certain number of laser photons can be a
bsorbed or emitted, yielding a spectrum of harmonics of the form omega (x)
= E-(p) over right arrow + nw(L) + I-io + U-p(tot), where E-(p) over right
arrow is the initial electron energy, It the number of emitted or absorbed
laser photons w(L), I-lo the ionization energy and U-p(tot) the total ponde
romotive energy of the bichromatic laser field. This process is of interest
for the generation of high=frequency fields during the laser heating of pl
asmas. We shall evaluate the nonlinear recombination probabilities as a fun
ction of the relative phase phi of the two field components using the inver
se form of the Keldysh-Faisal-Reiss model, also taking into account in an a
pproximate way the Coulomb effects of the ion on the recombining electron.
Moreover, we shall compare our quantum mechanical results with those obtain
ed from a classical theory of recombination, developed recently, based on B
ohr's correspondence principle.