1994
DOI: 10.1006/aphy.1994.1020
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The Electromagnetic Interactions of Electrons in the Lowest Landau Level

Abstract: Starting from a system of planar electrons in a strong magnetic field normal to the plane, interacting with perturbing electromagnetic fields, an effective Lagrangian for the fermions in the lowest Landau level (L.L.L.) has been derived. By choosing a suitable background electrostatic potential, an incompressible droplet of these electrons is constructed. The gauge invariant effective Lagrangian for the electrons in the L.L.L. is shown to split naturally into a $1+1$ dimensional Lagrangian for the electrons on… Show more

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Cited by 18 publications
(26 citation statements)
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“…The purely electromagnetic terms are familiar from previous studies concerning the electromagnetic effective action of spinless quantum Hall fermions. 16,17 From the effective action, we can readily compute the mean electromagnetic currents in the spin-textured ͑excited͒ state.…”
Section: ͑324͒mentioning
confidence: 99%
“…The purely electromagnetic terms are familiar from previous studies concerning the electromagnetic effective action of spinless quantum Hall fermions. 16,17 From the effective action, we can readily compute the mean electromagnetic currents in the spin-textured ͑excited͒ state.…”
Section: ͑324͒mentioning
confidence: 99%
“…The second term is the edge contribution. From (4.5) and (8.4), we see that This is just a chiral current moving with a velocity v = E B in agreement with [7], [8].…”
Section: Edge Current In a Quantum Hall Dropletmentioning
confidence: 69%
“…The effective action for planar electrons in a strong magnetic field coupled minimally to perturbative slowly-varying electromagnetic fields has already been given in [6], [7]. Here, we discuss the structure of the current operators arising from this effective action as a natural extension to what has been discussed in the earlier sections.…”
Section: Minimal Coupling To Electromagnetismmentioning
confidence: 85%
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“…Thus we have two von Neumann algebras, which become infinite dimensional as we take n → ∞. The state corresponding to (22), expressed in terms of the algebra as a density matrix, can be written, upon using (29), as…”
Section: The Spectrum Of the Modular Operator For The ν = 1 Hallmentioning
confidence: 99%