We calculate the localization corrections to the anomalous Hall conductivit
y related to the contribution of spin-orbit scattering into the, current ve
rtex (side-jump mechanism). We show that in contrast to the ordinary Hall e
ffect, there exists a nonvanishing localization correction to the anomalous
Hall resistivity. The correction to the anomalous Hall conductivity vanish
es in the case of side-jump mechanism, but is nonzero for the skew scatteri
ng. The total correction to the off-diagonal conductivity related to both m
echanisms, does not compensate the correction to the diagonal conductivity.