An universal description of the polarization bremsstrahlung of a fast charg
ed particle on a multielectron atom (Z much greater than 1, Z is the nuclea
r charge) is obtained using the local electron density method and the Thoma
s-Fermi statistical model. It is shown that the cross section of the proces
s can be represented in the form d sigma(PB)(omega) = Z(2)d<(sigma)over til
de>(PB)(nu), where the function d<(sigma)over tilde>(PB)(nu) exhibits appro
ximate scaling with respect to the parameter omega/Z = nu, and the correspo
nding R factor (ratio of the cross sections in the polarization and ordinar
y channels) is greater than 1 in a wide range of frequencies and reaches it
s maximum value at frequencies omega approximate to Z Ry. It is demonstrate
d that in the frequency range p(a)c < (h) over bar omega < gamma(2)p(a)c (g
amma is the relativistic factor, p(a) is the characteristic momentum of the
atomic electrons, and c is the speed of light) the angular distribution of
the polarization bremsstrahlung of a relativistic charged particle undergo
es narrowing due to the compensation, by the momentum of the emitted photon
, of the momentum transfer from the incident particle to the atomic core. (
C) 2000 MAIK "Nauka/Interperiodica".