Spontaneous Particle-Hole Symmetry Breaking in the ν=5/2 Fractional Quantum Hall Effect

Michael R. Peterson, Kwon Park, and S. Das Sarma
Phys. Rev. Lett. 101, 156803 – Published 8 October 2008

Abstract

The essence of the ν=5/2 fractional quantum Hall effect is believed to be captured by the Moore-Read Pfaffian (or anti-Pfaffian) description. However, a mystery regarding the formation of the Pfaffian state is the role of the three-body interaction Hamiltonian H3 that produces it as an exact ground state and the concomitant particle-hole symmetry breaking. We show that a two-body interaction Hamiltonian H2 constructed via particle-hole symmetrization of H3 produces a ground state nearly exactly approximating the Pfaffian and anti-Pfaffian states, respectively, in the spherical geometry. Importantly, the ground state energy of H2 exhibits a “Mexican-hat” structure as a function of particle number in the vicinity of half filling for a given flux indicating spontaneous particle-hole symmetry breaking. This signature is absent for the second Landau level Coulomb interaction at 5/2.

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  • Received 10 July 2008

DOI:https://doi.org/10.1103/PhysRevLett.101.156803

©2008 American Physical Society

Authors & Affiliations

Michael R. Peterson1, Kwon Park2, and S. Das Sarma1

  • 1Condensed Matter Theory Center, Department of Physics, University of Maryland, College Park, Maryland 20742, USA
  • 2School of Physics, Korea Institute for Advanced Study, Seoul 130-722, Korea

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Issue

Vol. 101, Iss. 15 — 10 October 2008

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