Theory of Incompressible States in a Narrow Channel
Tapash Chakraborty (1), K. Niemel\"a (2), P. Pietil\"ainen (2) ((1), Institute of Mathematical Sciences, Taramani, Madras, India (2) Theoretical, Physics, University of Oulu, Finland)

TL;DR
This paper explores the behavior of interacting electrons in a narrow quantum Hall channel, revealing abrupt changes in charge density profiles and identifying a new fractional quantum Hall state at half-filling.
Contribution
It introduces a phase diagram for narrow channels, including known odd-denominator states and a novel fractional quantum Hall state at half-filled Landau level.
Findings
Abrupt changes in charge-density profile width with Coulomb interaction strength
Identification of a new fractional quantum Hall state at half-filling
Similarity of collective mode to odd-denominator fractional quantum Hall states
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 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.
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