  We study the weak localization correction (WLC) to transport coefficients of
a system of electrons in a static long-range potential (e.g. an antidot array
or ballistic cavity). We found that the weak localization correction to the
current response is delayed by the large time $t_E = \lambda^{-1} |\ln \hbar|$,
where $\lambda$ is the Lyapunov exponent. In the semiclassical regime $t_E$ is
much larger than the transport lifetime. Thus, the fundamental characteristic
of the classical chaotic motion, Lyapunov exponent, may be found by measuring
the frequency or temperature dependence of WLC.
