Possibility of a Topological Phase Transition in Two-dimensional Model
arXiv:2112.15053 · doi:10.7566/JPSJ.92.114701
Abstract
We study by large-scale Monte Carlo simulation the model, which can be regarded as an effective low-energy model of a triangular lattice Heisenberg antiferromagnet. vortices appear as elementary excitations in the triangular lattice Heisenberg antiferromagnet. Such vortices are ubiquitous in other frustrated Heisenberg spin systems that have noncollinear long-range orders. In this study, we investigate a possible topological phase transition driven by the binding--unbinding of vortices. By extracting important degrees of freedom, we map a frustrated spin system to an effective model. From large-scale Monte Carlo simulation, we obtain an order parameter and a correlation length of up to . Concerning the existence of a -vortex transition, by extrapolating the order parameter to the thermodynamics limit assuming the -vortex transition, we obtain a finite transition temperature as . Our estimate of the correlation length at is much larger than , which is beyond the previous estimate obtained with the triangular lattice Heisenberg model.
arXiv comment7 pages, 8 figures, Added new analysis of the correlation length
References in corpus (8)
- Quantum Spin Ice: A Search for Gapless Quantum Spin Liquids in Pyrochlore Magnets
- Gapless spin-liquid ground state in the kagome antiferromagnet
- Z_2-vortex ordering of the triangular-lattice Heisenberg antiferromagnet
- Vortex-induced topological transition of the bilinear-biquadratic Heisenberg antiferromagnet on the triangular lattice
- Signature of a Z_2 vortex in the dynamical correlations of the triangular-lattice Heisenberg antiferromagnet
- Monte Carlo Simulation of the Heisenberg Antiferromagnet on a Triangular Lattice: Topological Excitations
- Spin-stiffness and topological defects in two-dimensional frustrated spin systems
- Two phase transitions in the two-dimensional nematic 3-vector model with no quasi long-range order: Monte Carlo simulation of the density of states