Lieb-Schultz-Mattis theorem with a local twist for general one-dimensional quantum systems
arXiv:1708.05186 · doi:10.1007/s10955-017-1946-0
Abstract
We formulate and prove the local twist version of the Yamanaka-Oshikawa-Affleck theorem, an extension of the Lieb-Schultz-Mattis theorem, for one-dimensional systems of quantum particles or spins. We can treat almost any translationally invariant system wth global symmetry. Time-reversal or inversion symmetry is not assumed. It is proved that, when the "filling factor" is not an integer, a ground state without any long-range order must be accompanied by low-lying excitations whose number grows indefinitely as the system size is increased. The result is closely related to the absence of topological order in one-dimension. The present paper is written in a self-contained manner, and does not require any knowledge of the Lieb-Schultz-Mattis and related theorems.
23 pages, 2 figures, minor changes in version 2
References in corpus (4)
Cited by in corpus (13)
- Lieb-Schultz-Mattis type theorems for quantum spin chains without continuous symmetry
- General Lieb-Schultz-Mattis type theorems for quantum spin chains
- Lieb-Schultz-Mattis type theorems for Majorana models with discrete symmetries
- Topological phase transition and index for quantum spin chains
- Lieb-Schultz-Mattis anomalies and web of dualities induced by gauging in quantum spin chains
- (SPT-)LSM theorems from projective non-invertible symmetries
- Lieb Schultz Mattis-Type Theorems and Other Non-perturbative Results for Strongly Correlated Systems with Conserved Dipole Moments
- Rigorous Index Theory for One-Dimensional Interacting Topological Insulators
- Non-perturbative approach to quantum liquid ground states on geometrically frustrated Heisenberg antiferromagnets
- Terminable Transitions in a Topological Fermionic Ladder
- Ground-State Phase Diagram of (1/2,1/2,1) Mixed Diamond Chains
- Interacting Crystalline Topological Insulators in two-dimensions with Time-Reversal Symmetry
- Anisotropy-induced spin parity effects