Abstract
We construct and analyze a frustrated quantum spin model with plaquette order, in which the low-energy dynamics is controlled by spin singlets. At a critical value of frustration the singlet spectrum becomes gapless, indicating a quantum transition to a phase with dimer order. The magnetic susceptibility has an activated form throughout the phase diagram, whereas the specific heat exhibits a rich structure and a power-law dependence on temperature at the quantum critical point. This generic behavior can be relevant to quantum antiferromagnets on Kagom\'e and pyrochlore lattices where (almost) all low-energy excitations are spin singlets, as well as to the ${\mathrm{CaV}}_{4}{\mathrm{O}}_{9}$ lattice and the strongly frustrated antiferromagnets ${\mathrm{Cu}}_{2}{\mathrm{Te}}_{2}{\mathrm{O}}_{5}(\mathrm{Cl},\mathrm{Br}{)}_{2}$ and ${\mathrm{Li}}_{2}\mathrm{VO}(\mathrm{Si},\mathrm{Ge}){\mathrm{O}}_{4}.$
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