  We introduce the concept of a bosonic spin liquid condensate (SLC), where
spinful bosons in a lattice form a zero-temperature spin disordered charge
condensate that preserves the spin rotation symmetry, but breaks the U(1)
symmetry due to a spinless order parameter with charge one. It has an energy
gap to all the spin excitations. We show that such SLC states can be realized
in a system of spin $S\ge 2$ bosons. In particular, we analyze the SLC phase
diagram in the spin 2 case using a mean-field variational wave function method.
We show there is a direct analogy between the SLC and the
resonating-valence-bond (RVB) state.
