Edge and impurity response in two-dimensional quantum antiferromagnets
arXiv:0808.0496 · doi:10.1103/PhysRevB.78.174410
Abstract
Motivated by recent Monte-Carlo simulations of Hoglund and Sandvik (arXiv:0808.0408), we study edge response in square lattice quantum antiferromagnets. We use the O(3) non-linear sigma-model to compute the decay asymptotics of the staggered magnetization, energy density and local magnetic susceptibility away from the edge. We find that the total edge susceptibility is negative and diverges logarithmically as the temperature vanishes. We confirm the predictions of the continuum theory by performing a 1/S expansion of the microscopic Heisenberg model with the edge. We propose a qualitative explanation of the edge dimerization seen in Monte-Carlo simulations by a theory of valence-bond-solid correlations in the Neel state. We also discuss the extension of the latter theory to the response of a single non-magnetic impurity, and its connection to the theory of the deconfined critical point.
25 pages, 6 figures
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- Effects of edge disorder in nano-scale antiferromagnetic clusters
- Spin correlations near the surface of a three-dimensional Heisenberg antiferromagnet
- Near-Boundary and Bulk Regions of a Semi-Infinite Two-Dimensional Heisenberg Antiferromagnet
- Many-body calculation of the spatial extent of the wave-function of a non-magnetic impurity in a d-wave high-temperature superconductor using the t--J model
- The t-J model on a semi-infinite lattice
- Excitations and spin correlations near the interface of two three-dimensional Heisenberg antiferromagnets