  We examine the idea, postulated by Phillips et al., that a finite resistivity
in $T \to 0$ limit in disordered granular superconducting (SC) films is
explained as a consequence of the absence of phase stiffness in a phase glass
(PG) peculiar to granular systems. It is found that a coupling between the
nonzero PG order and the ordinary SC fluctuation makes the conductivity
divergent. However, an actual drop of resistivity is argued to occur due to
another SC glass ordering, induced by the precursory PG fluctuation,
corresponding to the vortex-glass transition in a nonzero magnetic field.
