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Four-terminal resistance of a ballistic quantum wire

R. de Picciotto (), H. L. Stormer, L. N. Pfeiffer, K. W. Baldwin and K. W. West
Additional contact information
R. de Picciotto: Bell-Labs, Lucent Technologies
H. L. Stormer: Bell-Labs, Lucent Technologies
L. N. Pfeiffer: Bell-Labs, Lucent Technologies
K. W. Baldwin: Bell-Labs, Lucent Technologies
K. W. West: Bell-Labs, Lucent Technologies

Nature, 2001, vol. 411, issue 6833, 51-54

Abstract: Abstract The electrical resistance of a conductor is intimately related to the relaxation of the momentum of charge carriers. In a simple model, the accelerating force exerted on electrons by an applied electric field is balanced by a frictional force arising from their frequent collisions with obstacles such as impurities, grain boundaries or other deviations from a perfect crystalline order1. Thus, in the absence of any scattering, the electrical resistance should vanish altogether. Here, we observe such vanishing four-terminal resistance in a single-mode ballistic quantum wire. This result contrasts the value of the standard two-probe resistance measurements of h/2e2≈ 13 kΩ. The measurements are conducted in the highly controlled geometry afforded by epitaxial growth onto the cleaved edge of a high-quality GaAs/AlGaAs heterostructure. Two weakly invasive voltage probes are attached to the central section of a ballistic quantum wire to measure the inherent resistance of this clean one-dimensional conductor.

Date: 2001
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DOI: 10.1038/35075009

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