Lieb-Schultz-Mattis theorem for quasi-topological systems

dc.creatorFreedman, Michael
dc.creatorNayak, Chetan
dc.creatorShtengel, Kirill
dc.date2005-08-22
dc.date2008-11-27
dc.date.accessioned2026-07-07T12:04:54Z
dc.date.available2026-07-07T12:04:54Z
dc.descriptionIn this paper we address the question of the existence of a spectral gap in a class of local Hamiltonians. These Hamiltonians have the following properties: their ground states are known exactly; all equal-time correlation functions of local operators are short-ranged; and correlation functions of certain non-local operators are critical. A variational argument shows gaplessness with $ω\propto k^2$ at critical points defined by the absence of certain terms in the Hamiltonian, which is remarkable because equal-time correlation functions of local operators remain short-ranged. We call such critical points, in which spatial and temporal scaling are radically different, quasi-topological. When these terms are present in the Hamiltonian, the models are in gapped topological phases which are of special interest in the context of topological quantum computation.
dc.descriptionv2: The version published in Phys. Rev B. A new section has been added; a gap in the earlier version of the proof has been eliminated
dc.identifierhttps://arxiv.org/abs/cond-mat/0508508
dc.identifierhttp://arxiv.org/abs/cond-mat/0508508
dc.identifierPhys. Rev. B 78, 174411 (2008)
dc.identifierdoi:10.1103/PhysRevB.78.174411
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/208239
dc.subjectStrongly Correlated Electrons
dc.subjectStatistical Mechanics
dc.titleLieb-Schultz-Mattis theorem for quasi-topological systems
dc.typetext

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