Skyrmions of Frustrated Quantum Dimer Systems
cond-mat.str-el
Submitted: 2025-06-27
Updated: 2026-09-18
Comments: 17 pages, 12 figures
License: http://creativecommons.org/licenses/by/4.0/
The gist: Magnetic skyrmions are topologically protected solitons observed in various classes of real magnets.
Terminology
Abstract
Magnetic skyrmions are topologically protected solitons observed in various classes of real magnets. In two-dimensional systems, where the target space of local magnetization values is the two-sphere S squared, skyrmion textures are classified by the homotopy classes of two-loops S squared in S squared: Π 2(S 2) Z. Here, we demonstrate that more general topological skyrmion textures emerge in the classical limit of quantum dimer systems, where the phase space of the relevant classical theory is CP N-1 (with N=4 for the case of interest), because the relevant second homotopy group, Π 2(CP N-1) Z for N at least 2, remains unchanged. Building on the framework established by Zhang et al. (2023), we consider a classical limit based on SU(4) coherent states, which preserve intra-dimer entanglement. We show that the zero-temperature phase diagram of frustrated spin-dimer systems on a bilayer triangular lattice with weak inter-dimer coupling includes two magnetic-field-induced CP cubed skyrmion crystal phases.
Sources
- Langevin dynamics of generalized spins as SU($N$) coherent states
- Sunny.jl: A Julia Package for Spin Dynamics
- Spin dynamics of triple-Q magnetic orderings in a triangular lattice: Implications for multi-Q orderings in general two-dimensional lattices
Related papers
- Microscopic Constructions of the BF+AAB Topological Field Theory and Borromean-Rings Braiding in (3+1) Dimensions
- Transport in the emergent Bose liquid: Bad metal, strange metal, and weak insulator, all in one system
- Gibbs-state phases beyond microscopic symmetry breaking: A phase invariant for the 3D toric code
- Instabilities in self-consistent diagrammatic approaches and how to cure them
- True vs false Fermi surfaces in the Pseudogap regime and their transformation with doping and temperature in the Hubbard Model
- Orbital magnetic susceptibility and de Haas-van Alphen effect of a flat band from quantum geometry