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Degeneracy of non-Abelian quantum Hall states on the torus: domain walls and conformal field theory

Eddy Ardonne1,2, Emil J Bergholtz3, Janik Kailasvuori4 and Emma Wikberg3

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We analyze the non-Abelian Read–Rezayi quantum Hall states on the torus, where it is natural to employ a mapping of the many-body problem onto a one-dimensional lattice model. On the thin torus—the Tao–Thouless (TT) limit—the interacting many-body problem is exactly solvable. The Read–Rezayi states at filling ν = k/(kM+2) are known to be exact ground states of a local repulsive k+1-body interaction, and in the TT limit this is manifested in that all states in the ground state manifold have exactly k particles on any kM+2 consecutive sites. For M\neq 0 the two-body correlations of these states also imply that there is no more than one particle on M adjacent sites. The fractionally charged quasiparticles and quasiholes appear as domain walls between the ground states, and we show that the number of distinct domain wall patterns gives rise to the nontrivial degeneracies, required by the non-Abelian statistics of these states. In the second part of the paper we consider the quasihole degeneracies from a conformal field theory (CFT) perspective, and show that the counting of the domain wall patterns maps one to one on the CFT counting via the fusion rules. Moreover we extend the CFT analysis to topologies of higher genus.


Keywords

fractional QHE (theory)

conformal field theory (theory)

PACS

73.43.-f Quantum Hall effects

71.70.Di Landau levels

MSC

81V70 Many-body theory; quantum Hall effect

82B23 Exactly solvable models; Bethe ansatz

81T40 Two-dimensional field theories, conformal field theories, etc.

Subjects

Condensed matter: electrical, magnetic and optical

Surfaces, interfaces and thin films

Dates

Issue 04 (April 2008)

Received 13 February 2008, accepted for publication 19 March 2008

Published 14 April 2008



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