Projectification of point group symmetries with a background flux and Lieb-Schultz-Mattis theorem
arXiv:2505.00927 · doi:10.1103/8gq5-d954
Abstract
We discuss the Lieb-Schultz-Mattis (LSM) theorem in two-dimensional spin systems with on-site spin rotation symmetry and point group symmetry about a site. We ``twist" the point group symmetry by introducing a small uniform U(1) flux to obtain a projective symmetry, similarly to the familiar magnetic translation symmetry. The LSM theorem is proved in presence of the flux and then it is demonstrated that the theorem holds also for the flux-free system. Besides, the uniform flux enables us to show the LSM theorem for the time-reversal symmetry and the site-centered -rotation symmetry.
15 pages, 10 figures
References in corpus (11)
- Symmetric-Gapped Surface States of Fractional Topological Insulators
- Cyclic exchange, isolated states and spinon deconfinement in an XXZ Heisenberg model on the checkerboard lattice
- Topological Classification of Gapped Spin Chains :Quantized Berry Phase as a Local Order Parameter
- A Multi-Dimensional Lieb-Schultz-Mattis Theorem
- Twisted boundary condition and Lieb-Schultz-Mattis ingappability for discrete symmetries
- Geometric approach to Lieb-Schultz-Mattis theorem without translation symmetry under inversion or rotation symmetry
- Many-Body Chern Numbers of and States on Various Lattices
- Many-body multipole index and bulk-boundary correspondence
- Lieb-Schultz-Mattis theorem in higher dimensions from approximate magnetic translation symmetry
- Lieb-Schultz-Mattis Theorem for 1D Quantum Magnets with Antiunitary Translation and Inversion Symmetries
- Stability of quasi-particle creation and multiband geometry in fractional Chern insulators under magnetic fields