Solutions are obtained for the amplitudes of harmonics of focused wave beam
s in the paraxial approximation taking into account the self-action effects
caused by the third-order Ken nonlinearities. It is shown that the develop
ment of nonlinear processes is determined by the initial curvature of the w
ave front of the radiation at the fundamental frequency. As the intensity o
f the fundamental radiation in the media focusing this radiation is increas
ed, the harmonic signal can considerably increase in intensity for a medium
initial focusing and oscillate for weak and strong focusing. For the media
defocusing the fundamental radiation or changing the dielectric constant a
t the harmonic frequency, the power dependence of the intensity of higher h
armonics on the intensity of fundamental radiation becomes weaker. The resu
lts of the present work are compared with the experimental data on harmonic
generation in gases.