Deconfined Quantum Critical Point on the Triangular Lattice
arXiv:1710.04668 · doi:10.1103/PhysRevB.97.195115
Abstract
We first propose a topological term that captures the "intertwinement" between the standard "" antiferromagnetic order (or the so-called 120 state) and the "" valence solid bond (VBS) order for spin-1/2 systems on a triangular lattice. Then using a controlled renormalization group calculation, we demonstrate that there exists an unfine-tuned direct continuous deconfined quantum critical point (dQCP) between the two ordered phases mentioned above. This dQCP is described by the quantum electrodynamics (QED) with an emergent PSU(4)=SU(4)/ symmetry only at the critical point. The topological term aforementioned is also naturally derived from the QED. We also point out that physics around this dQCP is analogous to the boundary of a bosonic symmetry protected topological state with on-site symmetries only.
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