Dissipative Quantum Hall Effect in Graphene near the Dirac Point
arXiv:cond-mat/0702125 · doi:10.1103/PhysRevLett.98.196806
Abstract
We report on the unusual nature of nu=0 state in the integer quantum Hall effect (QHE) in graphene and show that electron transport in this regime is dominated by counter-propagating edge states. Such states, intrinsic to massless Dirac quasiparticles, manifest themselves in a large longitudinal resistivity rho_xx > h/e^2, in striking contrast to rho_xx behavior in the standard QHE. The nu=0 state in graphene is also predicted to exhibit pronounced fluctuations in rho_xy and rho_xx and a smeared zero Hall plateau in sigma_xy, in agreement with experiment. The existence of gapless edge states puts stringent constraints on possible theoretical models of the nu=0 state.
4 pgs, 4 fgs
References in corpus (2)
Cited by in corpus (13)
- AC conductivity of graphene: from tight-binding model to 2+1-dimensional quantum electrodynamics
- The zero-energy state in graphene in a high magnetic field
- Theory of Anomalous Quantum Hall Effects in Graphene
- Quantum-Hall activation gaps in graphene
- SO(3) symmetry between Neel and ferromagnetic order parameters for graphene in a magnetic field
- Conformal Invariance and Shape-Dependent Conductance of Graphene Samples
- Charge and Spin Transport at the Quantum Hall Edge of Graphene
- Dynamics in the quantum Hall effect and the phase diagram of graphene
- Edge states, mass and spin gaps, and quantum Hall effect in graphene
- Dissipation and criticality in the lowest Landau level of graphene
- Toward theory of quantum Hall effect in graphene
- Edge states in graphene in magnetic fields -- a speciality of the edge mode embedded in the n=0 Landau band
- Quantum Hall ferromagnetism in graphene: a SU(4) bosonization approach