  We employ a recently developed computational many-body technique to study for
the first time the half-filled Anderson-Hubbard model at finite temperature and
arbitrary correlation ($U$) and disorder ($V$) strengths. Interestingly, the
narrow zero temperature metallic range induced by disorder from the Mott
insulator expands with increasing temperature in a manner resembling a quantum
critical point. Our study of the resistivity temperature scaling $T^{\alpha}$
for this metal reveals non Fermi liquid characteristics. Moreover, a continuous
dependence of $\alpha$ on $U$ and $V$ from linear to nearly quadratic was
observed. We argue that these exotic results arise from a systematic change
with $U$ and $V$ of the "effective" disorder, a combination of quenched
disorder and intrinsic localized spins.
