The mean-field theory of static and dynamic properties of the Dzyalosh
inskii-Moriya (DM) interaction in Heisenberg spin glasses is developed
. The main idea of the paper is based on the property of microscopic D
M vectors D(ij) describing this interaction: each vector D(ij) is defi
ned up to a sign. It is a reason for the existence of additional degre
es of freedom connected with ordering of vectors D(ij) on orientations
below the freezing temperature. The theory is formulated on the basis
of the eigenmodes of the exchange integrals matrix J(ij). There are t
wo additional important assumptions to define the model. The first one
is the independence of the sum SIGMA(i) J(ij) from the index j that r
estricts possible distributions of random exchange integrals. However,
due to this assumption the total magnetization appears to be a hard e
igenmode of the exchange part of the Hamiltonian and it is possible to
a great extent to escape a detailed consideration of the spin-glass t
ransition as well as to separate terms containing magnetization vector
s in an equation for the thermodynamic potential in explicit form. The
description of ordering of DM vectors D(ij) is carried out in terms o
f some effective paramagnetic pseudospin, of which the state depends o
n the thermodynamic path of the spin-glass sample. This property displ
ays itself in the distinction between the field and zero-field-cooling
susceptibility and in an appearance of the macroscopical unidirection
al anisotropy field (the DM field). The second assumption is to consid
er the DM field as a slow dynamical variable with a broad spectrum of
relaxation times which, however, can behave as a quenched quantity at
low enough temperatures. Motion equations of a dissipative character f
or pseudospins are examined. Pseudospins corresponding to localized ei
genmodes with characterizing size xi approximately 10(2) - 10(3) angst
rom effectively contribute to observable slow relaxation. Using the dy
namic susceptibility calculated the frequency dependence of freezing t
emperature and the magnetization decay law are found.