Phase structure of gauge theories for frustrated antiferromagnets in two dimensions
arXiv:0909.5030 · doi:10.1103/PhysRevB.80.224425
Abstract
In this paper, we study phase structure of lattice gauge theories that appear as an effective field theory describing low-energy properties of frustrated antiferromagnets in two dimensions. Spin operators are expressed in terms of Schwinger bosons, and an emergent U(1) gauge symmetry reduces to a gauge symmetry as a result of condensation of a bilinear operator of the Schwinger boson describing a short-range spiral order. We investigated the phase structure of the gauge theories by means of the Monte-Carlo simulations, and found that there exist three phases, phase with a long-range spiral order, a dimer state, and a spin liquid with deconfined spinons. Detailed phase structure and properties of phase transitions depend on details of the models.
11 pages, 27 figures, Version to be published in Phys.Rev.B
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Cited by in corpus (4)
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- Deconfined criticality for the S=1 spin model on the spatially anisotropic triangular lattice
- Phase Structure of Anisotropic Antiferromagnetic Heisenberg Model on Layered Triangular Lattice: Spiral State and Deconfined Spin Liquid
- Sign-problem-free effective models of triangular lattice quantum antiferromagnets