We report on a systematic study of two-dimensional, periodic, frustrated Is
ing models with quantum dynamics introduced via a transverse magnetic field
. The systems studied are the triangular and kagome lattice antiferromagnet
s, fully frustrated models on the square and hexagonal (honeycomb) lattices
, a planar analog of the pyrochlore antiferromagnet, a pentagonal lattice a
ntiferromagnet. as well as two quasi-one-dimensional lattices that have con
siderable pedagogical value. All of these exhibit a macroscopic degeneracy
at T = 0 in the absence of the transverse field, which enters as a singular
perturbation. We analyze these systems with a combination of a variational
method at weak fields, a perturbative Landau-Ginzburg-Wilson approach from
large fields, as well as quantum Monte Carlo simulations utilizing a clust
er algorithm. Our results include instances of quantum order arising from c
lassical criticality (triangular lattice) or classical disorder (pentagonal
and probably hexagonal) as well as notable instances of quantum disorder a
rising from classical disorder (kagome). We also discuss the effect of fini
te temperature, as well as the interplay between longitudinal and transvers
e fields-in the kagome problem the latter gives rise to a nontrivial phase
diagram with bond-ordered and bond-critical phases in addition to the disor
dered phase. We also note connections to quantum-dimer models and thereby t
o the physics of Heisenberg antiferromagnets in short-ranged resonating val
ence-bond phases that have been invoked in discussions of high-temperature
superconductivity.