arXiv Analytics

Sign in

arXiv:cond-mat/9807241AbstractReferencesReviewsResources

(Mis-)handling gauge invariance in the theory of the quantum Hall effect III: The instanton vacuum and chiral edge physics

A. M. M. Pruisken, B. Skoric, M. A. Baranov

Published 1998-07-16, updated 1999-04-29Version 4

The concepts of an instanton vacuum and F-invariance are used to derive a complete effective theory of massless edge excitations in the quantum Hall effect. We establish, for the first time, the fundamental relation between the instanton vacuum approach and the theory of chiral edge bosons. Two longstanding problems of smooth disorder and Coulomb interactions are addressed. We introduce a two dimensional network of chiral edge states and tunneling centers (saddlepoints) as a model for the plateau transitions. We derive a mean field theory including the Coulomb interactions and explain the recent empirical fits to transport at low temperatures. Secondly, we address the problem of electron tunneling into the quantum Hall edge. We express the problem in terms of an effective Luttinger liquid with conductance parameter (g) equal to the filling fraction (\nu) of the Landau band. Hence, even in the integral regime our results for tunneling are completely non-Fermi liquid like, in sharp contrast to the predictions of single edge theories.

Comments: 51 pages, 8 figures; section IIA3 completely revised, section IIB and appendix C corrected; submitted to Phys.Rev.B
Journal: Phys.Rev.B60:16838-16864,1999
Categories: cond-mat.mes-hall
Related articles: Most relevant | Search more
arXiv:cond-mat/0011410 (Published 2000-11-23)
The problem of Coulomb interactions in the theory of the quantum Hall effect
arXiv:0810.1494 [cond-mat.mes-hall] (Published 2008-10-08, updated 2009-08-02)
Quantum Hall Effect in Bilayer Graphene: Disorder Effect and Quantum Phase Transition
arXiv:cond-mat/9712322 (Published 1997-12-30, updated 1999-04-29)
(Mis-)handling gauge invariance in the theory of the quantum Hall effect I: Unifying action and the ν=1/2 state