Magnetoelasticity theory of incompressible quantum Hall liquids

dc.creatorTokatly, I. V.
dc.date2005-05-30
dc.date2006-05-19
dc.date.accessioned2026-07-07T06:37:53Z
dc.date.available2026-07-07T06:37:53Z
dc.descriptionA simple and physically transparent magnetoelasticity theory is proposed to describe linear dynamics of incompressible fractional quantum Hall states. The theory manifestly satisfies the Kohn theorem and the $f$-sum rule, and predicts a gaped intra-Landau level collective mode with a roton minimum. In the limit of vanishing bare mass $m$ the correct form of the static structure factor, $s(q)\sim q^4$, is recovered. We establish a connection of the present approach to the fermionic Chern-Simons theory, and discuss further extensions and applications. We also make an interesting analogy of the present theory to the theory of visco-elastic fluids.
dc.descriptionRevTeX 4, 6 pages; expanded version to appear in PRB; more technical details, and discussions of the physics added
dc.identifierhttps://arxiv.org/abs/cond-mat/0505715
dc.identifierhttp://arxiv.org/abs/cond-mat/0505715
dc.identifierPhys. Rev. B 73, 205340 (2006)
dc.identifierdoi:10.1103/PhysRevB.73.205340
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/100549
dc.subjectMesoscale and Nanoscale Physics
dc.subjectStrongly Correlated Electrons
dc.titleMagnetoelasticity theory of incompressible quantum Hall liquids
dc.typetext

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