Supersymmetry and Correlated Electrons in Graphene Quantum Hall Effect

dc.creatorEzawa, Motohiko
dc.date2006-09-24
dc.date.accessioned2026-07-07T08:49:07Z
dc.date.available2026-07-07T08:49:07Z
dc.descriptionWe present a supersymmetric description of the quantum Hall effect (QHE) in graphene. The noninteracting system is supersymmetric separately at the so-called K and K' points of the Brillouin zone corners. Its essential consequence is that the energy levels and the Landau levels are different objects in graphene QHE. Each energy level has a four-fold degeneracy within the noninteracting theory. With the Coulomb interaction included, an excitonic gap opens in the zero-energy state, while each nonzero energy level splits into two levels since up-spin and down-spin electrons come from different Landau levels. We argue the emergence of the plateaux at $ν=\pm (4n-2)$ for small magnetic field $B$ and at $ν=0$, $\pm 1$, $\pm 2n$ for large $B$ with $n$ natural numbers.
dc.description5 pages, 2 figures
dc.identifierhttps://arxiv.org/abs/cond-mat/0609612
dc.identifierhttp://arxiv.org/abs/cond-mat/0609612
dc.identifierPhysica E 40, 269 (2007)
dc.identifierdoi:10.1016/j.physe.2007.06.038
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/144184
dc.subjectMesoscale and Nanoscale Physics
dc.subjectStrongly Correlated Electrons
dc.titleSupersymmetry and Correlated Electrons in Graphene Quantum Hall Effect
dc.typetext

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