Liquid-Crystal State of $ν=1/m$ Quantum Hall Effects

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dc.creatorBalev, O. G.
dc.date2005-01-20
dc.date2005-06-27
dc.date.accessioned2026-07-07T03:03:22Z
dc.date.available2026-07-07T03:03:22Z
dc.descriptionAt filling factor $ν=1/m$, $m$ odd integer, I present variational ground-state and excited-state wave functions, of two-dimensional electron system with homogeneous ion background, that show the condensation into a liquid-crystal state. For $m=1, 3, 5$, the ground-state energy per electron is substantially lower than the Laughlin one, for uniform liquid state.
dc.description4 pages; shorter version, resubmitted to Phys. Rev. Lett.; some explanations are added
dc.identifierhttps://arxiv.org/abs/cond-mat/0501507
dc.identifierhttp://arxiv.org/abs/cond-mat/0501507
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/25726
dc.subjectMesoscale and Nanoscale Physics
dc.subjectStrongly Correlated Electrons
dc.titleLiquid-Crystal State of $ν=1/m$ Quantum Hall Effects
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