Quantum Hall States at $ν=\frac{2}{k+2}$

dc.creatorBishara, Waheb
dc.creatorFiete, Gregory A.
dc.creatorNayak, Chetan
dc.date2008-04-11
dc.date2008-04-17
dc.date.accessioned2026-07-07T09:47:18Z
dc.date.available2026-07-07T09:47:18Z
dc.descriptionWe study the $ν=\frac{2}{k+2}$ quantum Hall states which are particle-hole conjugates of the $ν=\frac{k}{k+2}$ Read-Rezayi states. We find that equilibration between the different modes at the edge of such a state leads to an emergent SU(2)$_k$ algebra in the counter-propagating neutral sector. Heat flow along the edges of these states will be in the opposite direction of charge flow. In the $k=3$ case, which may be relevant to $ν=2+{2/5}$, the thermal Hall conductance and the exponents associated with quasiparticle and electron tunneling distinguish this state from competing states such as the hierarchy/Jain state.
dc.description4 pages
dc.identifierhttps://arxiv.org/abs/0804.1960
dc.identifierhttp://arxiv.org/abs/0804.1960
dc.identifierPhys. Rev. B 77, 241306(R) (2008), Editor's Suggestion
dc.identifierdoi:10.1103/PhysRevB.77.241306
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/163826
dc.subjectMesoscale and Nanoscale Physics
dc.subjectStrongly Correlated Electrons
dc.titleQuantum Hall States at $ν=\frac{2}{k+2}$
dc.typetext

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