We discuss the phase diagram of the quantum dimer model on the hexagonal (h
oneycomb) lattice. In addition to the columnar and staggered valence-bond s
olids which have been discussed in previous work, we establish the existenc
e of a plaquette valence-bond solid. The transition between the plaquette a
nd columnar phases at v/t = -0.2+/-0.05 is argued to be first order. We not
e that this model should describe valence-bond-dominated phases of frustrat
ed Heisenberg models on the hexagonal lattice and discuss its relation to r
ecent exact diagonalization work by Fouet et al. on the J(1)-J(2) model on
the same lattice. Our results also shed light on the properties of the tran
sverse field Ising antiferromagnet on the triangular lattice and the classi
cal [sing antiferromagnet on the stacked triangular lattice, which are rela
ted to dimer models by duality.