First order rotational perturbations of the fiat Friedmann-Robertson-Walker
metric are considered in the framework of four dimensional Neveu-Schwarz-N
eveu-Schwarz string cosmological models coupled with dilaton and axion fiel
ds. For the H field we use the solitonic ansatz, assuming that it is a func
tion of time only. The decay rate of rotation depends mainly upon the dilat
on field potential U. The equation for rotation imposes strong limitations
upon the functional form of U, restricting the allowed potentials to two: t
he trivial case U=0 and a generalized exponential type potential. In these
two models the metric rotation function can be obtained in an ex;lct analyt
ic form in both Einstein and string frames. In the potential-free case the
decay of rotational perturbations is governed by an arbitrary function of t
ime while in the presence of a potential the rotation tends rapidly to zero
in both Einstein and string frames.