Theory of Incompressible States in a Narrow Channel

Tapash Chakraborty, K. Niemelä, and P. Pietiläinen
Phys. Rev. Lett. 78, 4829 – Published 23 June 1997
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Abstract

We report on the properties of a system of interacting electrons in a narrow channel in the quantum Hall effect regime. It is shown that an increase in the strength of the Coulomb interaction causes abrupt changes in the width of the charge-density profile of translationally invariant states. We derive a phase diagram which includes many of the stable odd-denominator states as well as a novel fractional quantum Hall state at the lowest half-filled Landau level. The collective mode evaluated at the half-filled case is strikingly similar to that for an odd-denominator fractional quantum Hall state.

  • Received 2 December 1996

DOI:https://doi.org/10.1103/PhysRevLett.78.4829

©1997 American Physical Society

Authors & Affiliations

Tapash Chakraborty

  • Institute of Mathematical Sciences, Taramani, Madras 600 113, India

K. Niemelä and P. Pietiläinen

  • Theoretical Physics, University of Oulu, Linnanmaa, FIN-90570 Oulu, Finland

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Vol. 78, Iss. 25 — 23 June 1997

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