  Gapped $Z_{2}$ spin liquid as the simplest spin liquid has been proved to be
the most difficult to realize in realistic models. Here we show that the
frustration from a third-neighbor exchange $J_{3}$ on the spin-$\frac{1}{2}$
$J_{1}-J_{2}$ model on the square lattice may serve to stabilize such a
long-sought state. We argue that a Bosonic RVB description is more appropriate
than a Fermonic RVB description for such a gapped spin liquid phase. We show
that while the mean field ansatz of the proposed state has a $U(1)$ gauge
symmetry, the gauge fluctuation spectrum on it is actually gapped and the state
should be understood rather as a $Z_{2}$ spin liquid state with topological
order. The state is thus locally stable with respect to gauge fluctuation and
can emerge continuously from a collinear Neel ordered phase.
