Reconciling edge states with compressible stripes in a ballistic mesoscopic conductor
arXiv:1903.05028 · doi:10.1088/2515-7639/ab7582
Abstract
The well-known Landauer-Buttiker (LB) picture used to explain the quantum Hall effect uses the concept of (chiral) edge states that carry the current. In their seminal 1992 article, Chklovskii, Shklovskii and Glazman (CSG) showed that the LB picture does not account for some very basic properties of the gas, such as its density profile, as it lacks a proper treatment of the electrostatic energy. They showed that, instead, one should consider alternated stripes of compressible and incompressible phases. In this letter, we revisit this issue using a full solution of the quantum-electrostatic problem of a narrow ballistic conductor, beyond the CSG approach. We recover the LB channels at low field and the CSG compressible/incompressible stripes at high field. Our calculations reveal the existence of a third "hybrid" phase at intermediate field. This hybrid phase has well defined LB type edge states, yet possesses a Landau level pinned at the Fermi energy as in the CSG picture. We calculate the magneto-conductance which reveals the interplay between the LB and CSG regimes. Our results have important implications for the propagation of edge magneto-plasmons.
arXiv comment6 pages, 3 figures
References in corpus (15)
- The microscopic nature of localization in the quantum Hall effect
- Incompressible strips in dissipative Hall bars as origin of quantized Hall plateaus
- Self-consistent local-equilibrium model for density profile and distribution of dissipative currents in a Hall bar under strong magnetic fields
- Voltage-controlled Group Velocity of Edge Magnetoplasmon in the Quantum Hall Regime
- Thomas-Fermi-Poisson theory of screening for latterally confined and unconfined two-dimensional electron systems in strong magnetic fields
- Unveiling the bosonic nature of an ultrashort few-electron pulse
- Imaging the Conductance of Integer and Fractional Quantum Hall Edge States
- Anatomy of the quantum melting of the two dimensional Wigner crystal
- The self-consistent quantum-electrostatic problem in strongly non-linear regime
- Evolution of the quantum Hall bulk spectrum into chiral edge states
- Optimization of edge state velocity in the integer quantum Hall regime
- Self-consistent Coulomb picture of an electron-electron bilayer system
- Current-induced asymmetries of incompressible stripes in narrow quantum Hall systems
- Exchange-correlation enhancement of the Lande-g* factor in integer quantized Hall plateaus
- Edge electrostatics revisited
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- Electrostatics in semiconducting devices I : The Pure Electrostatics Self Consistent Approximation