  Electric resistivity, specific heat, magnetic susceptibility, and inelastic
neutron scattering experiments were performed on a single crystal of the heavy
fermion compound Ce(Ni$_{0.935}$Pd$_{0.065}$)$_2$Ge$_2$ in order to study the
spin fluctuations near an antiferromagnetic (AF) quantum critical point (QCP).
The resistivity and the specific heat coefficient for $T \leq$ 1 K exhibit the
power law behavior expected for a 3D itinerant AF QCP ($\rho(T) \sim T^{3/2}$
and $\gamma(T) \sim \gamma_0 - b T^{1/2}$). However, for 2 $\leq T \leq$ 10 K,
the susceptibility and specific heat vary as $log T$ and the resistivity varies
linearly with temperature. Furthermore, despite the fact that the resistivity
and specific heat exhibit the non-Fermi liquid behavior expected at a QCP, the
correlation length, correlation time, and staggered susceptibility of the spin
fluctuations remain finite at low temperature. We suggest that these deviations
from the divergent behavior expected for a QCP may result from alloy disorder.
