  We study the conductivity of a 3D disordered metal close to the
antiferromagnetic instability within the framework of the spin-fermion model
using the diagrammatic technique. We calculate the interaction correction
$\delta\sigma(\omega,T)$ to the conductivity, assuming that the latter is
dominated by the disorder scattering, and the interaction is weak. Although the
fermionic scattering rate shows critical behaviour on the entire Fermi surface,
the interaction correction is dominated by the processes near the hot spots,
narrow regions of the Fermi-surface corresponding to the strongest spin-fermion
scattering. Exactly at the critical point $\delta\sigma\propto[max(\omega,
T)]^{3/2}$. At sufficiently large frequencies $\omega$ the conductivity is
independent of the temperature, and
$\delta\sigma\propto(\tau^{-1}-i\omega)^{-2}$, $\tau$ being the elastic
scattering time. In a certain intermediate frequency range
$\delta\sigma(\omega)\propto i\omega(\tau^{-1}-i\omega)^{-2}$.
