  We analyze the anisotropic Kardar-Parisi-Zhang equation in general substrate
dimensions $d'$ with spatially correlated noise, $\langle\tilde
\eta({\bf{k}},\omega)\rangle=0$ and $\langle\tilde \eta({\bf{k}},\omega) \tilde
\eta({\bf{k}}',\omega')\rangle$
$=2D(k)\delta^{d'}({\bf{k}}+{\bf{k}}')\delta(\omega+\omega')$ where
$D(k)=D_0+D_{\rho}k^{-2\rho}$, using the dynamic renormalization group (RG)
method. When the signs of the nonlinear terms in parallel and perpendicular
directions are opposite, a novel finite stable fixed point is found for $d'<
d'_c \equiv 2+2\rho$ within one-loop order. The roughening exponent $\alpha$
and the dynamic exponent $z$ associated with the stable fixed point are
determined as $\alpha={2 \over 3}\big(\rho-{{d'-2}\over 2}\big)$, and
$z=2-\alpha$. For $d' > d'_c$, the RG transformations flow to the fixed point
of the weak-coupling limit, so that the dynamic exponent becomes $z=2$.

Condensed Matter