Fractional quantum Hall effect in graphene

C. Töke, Paul E. Lammert, Vincent H. Crespi, Jainendra K. Jain

Research output: Contribution to journalArticle

119 Citations (Scopus)

Abstract

Unlike regular electron spin, the pseudospin degeneracy of Fermi points in graphene does not couple directly to magnetic field. Therefore graphene provides a natural vehicle to observe the integral and fractional quantum Hall physics in an elusive limit analogous to zero Zeeman splitting in GaAs systems. This limit can exhibit new integral plateaus arising from interactions, large pseudoskyrmions, fractional sequences, even/odd numerator effects, composite-fermion pseudoskyrmions, and a pseudospin-singlet composite-fermion Fermi sea. It is stressed that the Dirac nature of the B=0 spectrum, which induces qualitative changes in the overall spectrum, has no bearing on the fractional quantum Hall effect in the n=0 Landau level of graphene. The second Landau level of graphene is predicted to show more robust fractional quantum Hall effect than the second Landau level of GaAs.

Original languageEnglish
Article number235417
JournalPhysical Review B - Condensed Matter and Materials Physics
Volume74
Issue number23
DOIs
Publication statusPublished - 2006

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Quantum Hall effect
Graphite
quantum Hall effect
Graphene
graphene
Fermions
Bearings (structural)
fermions
composite materials
Composite materials
electron spin
plateaus
vehicles
Physics
Magnetic fields
physics
Electrons
magnetic fields
interactions
gallium arsenide

ASJC Scopus subject areas

  • Condensed Matter Physics

Cite this

Fractional quantum Hall effect in graphene. / Töke, C.; Lammert, Paul E.; Crespi, Vincent H.; Jain, Jainendra K.

In: Physical Review B - Condensed Matter and Materials Physics, Vol. 74, No. 23, 235417, 2006.

Research output: Contribution to journalArticle

Töke, C. ; Lammert, Paul E. ; Crespi, Vincent H. ; Jain, Jainendra K. / Fractional quantum Hall effect in graphene. In: Physical Review B - Condensed Matter and Materials Physics. 2006 ; Vol. 74, No. 23.
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