On the basis of the method of reduced Rayleigh equations we present a
simple and reciprocal theory of the coherent and incoherent scattering
of x-rays from one- and two-dimensional randomly rough surfaces, that
appears to be free from the limitations of earlier theories of such s
cattering based on the Born and distorted-wave Born approximations. In
our approach, the reduced Rayleigh equation for the scattering amplit
ude(s) is solved perturbatively, with the small parameter of the theor
y eta(omega) = 1 - epsilon(omega), where epsilon(omega) is the dielect
ric function of the scattering medium. The magnitude of eta(omega) for
x-rays is in the range from 10(-6) to 10(-3) depending on the wavelen
gth of the x-rays. The contributions to the mean differential reflecti
on coefficient from the coherent and incoherent components of the scat
tered x-rays are calculated through terms of second order in eta(omega
). The resulting expressions are valid to all orders in the surface pr
ofile function. The results for the incoherent scattering display a Yo
neda peak when the scattering angle equals the critical angle for tota
l internal reflection from the vacuum-scattering medium interface for
a fixed angle of incidence, and when the angle of incidence equals the
critical angle for total internal reflection for a fixed scattering a
ngle. The approach used here may also be useful in theoretical studies
of the scattering of electromagnetic waves from randomly rough dielec
tric-dielectric interfaces, when the difference between the dielectric
constants on the two sides of the interface is small.