Invariance of Charge of Laughlin Quasiparticles
arXiv:cond-mat/0010093 · doi:10.1103/PhysRevB.64.085319
Abstract
A Quantum Antidot electrometer has been used in the first direct observation of the fractionally quantized electric charge. In this paper we report experiments performed on the integer i = 1, 2 and fractional f = 1/3 quantum Hall plateaus extending over a filling factor range of at least 27%. We find the charge of the Laughlin quasiparticles to be invariantly e/3, with standard deviation of 1.2% and absolute accuracy of 4%, independent of filling, tunneling current, and temperature.
4 pages, 5 figs
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- Conductance of one-dimensional quantum wires
- Coulomb blockade of anyons
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- Coulomb Oscillations in Antidots in the Integer and Fractional Quantum Hall Regimes
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- Superperiods and quantum statistics of Laughlin quasiparticles
- Possible observation of phase coexistence of the fractional quantum Hall liquid and a solid
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- Strong-coupling branching of FQHL edges
- Antidot tunneling between Quantum Hall liquids with different filling factors
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- Effective theory of fractional topological insulators in two spatial dimensions
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- Orbital Kondo effect in fractional quantum Hall systems
- Correlated transport of FQHE quasiparticles in a double-antidot system
- Experimental realization of Laughlin quasiparticle interferometers
- Energy spectrum of a 2D Dirac oscillator in the presence of a constant magnetic field and an antidot potential
- Quantum computation with hybrid parafermion-spin qubits
- Coulomb oscillations of a quantum antidot formed by an airbridged pillar gate in the integer and fractional quantum Hall regime