We consider (2 + 1)-dimensional beams, whose transverse size may be compara
ble to or smaller than the carrier wavelength, on the basis of an extended
version of the nonlinear Schrodinger equation derived from Maxwell's equati
ons. As this equation is very cumbersome, we also study, in parallel, its s
implified version, which keeps the most essential term, namely the term tha
t accounts for the nonlinear diffraction. The full equation additionally in
cludes terms generated by a deviation from the paraxial approximation and b
y a longitudinal electric-field component in the beam. Solitary-wave statio
nary solutions to both the full and simplified equations are found, treatin
g the terms that modify the nonlinear Schrodinger equation as perturbations
. Within the framework of the perturbative approach, a conserved power of t
he beam is obtained in an explicit form. It is found that the nonlinear dif
fraction affects stationary beams Much stronger than nonparaxiality and lon
gitudinal field. Stability of the beams is directly tested by simulating th
e simplified equation, with initial configurations taken as predicted by th
e perturbation theory. The numerically generated solitary beams are always
stable and never start to collapse, although they display periodic internal
vibrations, whose amplitude decreases with the increase of the beam power.