  AKLT state (or Haldane phase) in a spin-1 chain represents a large class of
gapped topological paramagnets, which hosts symmetry-protected gapless
excitations on the boundary. In this work we show how to realize this type of
featureless spin-1 states on a generic two-dimensional lattice. These states
have a gapped spectrum in the bulk but supports gapless edge states protected
by spin rotational symmetry along a certain direction, and are featured by spin
quantum Hall effect. Using fermion representation of integer-spins we show a
concrete example of such spin-1 topological paramagnets on kagome lattice, and
suggest a microscopic spin-1 Hamiltonian which may realize it.
