A simplified form of multiphoton and tunneling ionization is applied t
o the problem of ionization of atoms by a bichromatic field consisting
of the coherent superposition of a fundamental field and its second h
armonic: E(t)=0.5[E1 exp(-iomegat) + E2 exp(-2iomegat)] + c.c. This su
perposition possesses a polar asymmetric average of the cube of the fi
eld, [E3]=3/8(E1(2) E2 + E1(2)E2*). Two limits of the adiabaticity pa
rameter gamma are considered, where gamma=omega(2mI)1/2/(Absolute of v
alue of e E) and I is the ionization potential. The case gamma << 1 co
rresponds to tunneling ionization by a quasistatic field. Here, the el
ectron is released from the barrier with almost. zero velocity at the
moment when the magnitude of the field strength Absolute value of E is
maximum. Subsequent oscillations of the free electron in the strong b
ut adiabatically decreasing field yield some residual velocity. Polar
asymmetry of the distribution of that velocity and [v] are calculated
as a function of the phase shift, arg(E1(2)E2), between the squared f
undamental field E1(2) and its second harmonic E2. The other case, gam
ma >> 1, corresponds to multiphoton ionization by the combined fields
where n1HBARomega + n(2)2HBARomega almost-equal-to I. Interference of
the amplitudes corresponding to opposite parities of the total number
of quanta n1 + n2 with the same energy (n1 + 2n2)=const (almost-equal-
to I/HBARomega) gives rise to the arg(E1(2)E2)-dependent polar asymme
try of emitted electrons. Recent experiments on arg(E1(2)E2)-sensitiv
e effects in multiphoton ionization are discussed.