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Phys. Rev. B 73, 245115 (2006) [10 pages]

Entanglement entropy and the Berry phase in the solid state

S. Ryu
Kavli Institute for Theoretical Physics, University of California, Santa Barbara, California 93106, USA

Y. Hatsugai
Department of Applied Physics, University of Tokyo, Hongo Bunkyo-ku, Tokyo 113-8656, Japan
Received 11 January 2006; revised 16 May 2006; published 26 June 2006

The entanglement entropy (von Neumann entropy) has been used to characterize the complexity of many-body ground states in strongly correlated systems. In this paper, we try to establish a connection between the lower bound of the von Neumann entropy and the Berry phase defined for quantum ground states. As an example, a family of translational invariant lattice free fermion systems with two bands separated by a finite gap is investigated. We argue that, for one-dimensional (1D) cases, when the Berry phase (Zak's phase) of the occupied band is equal to pi×(odd  integer) and when the ground state respects a discrete unitary particle-hole symmetry (chiral symmetry), the entanglement entropy in the thermodynamic limit is at least larger than ln 2 (per boundary), i.e., the entanglement entropy that corresponds to a maximally entangled pair of two qubits. We also discuss how this lower bound is related to vanishing of the expectation value of a certain nonlocal operator which creates a kink in 1D systems.

©2006 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevB.73.245115
DOI: 10.1103/PhysRevB.73.245115
PACS: 71.10.Fd; 73.43.-f; 03.65.Ud; 77.22.Ej
  • 71.10.Fd
    Lattice fermion models (condensed matter) including Hubbard model, etc
  • 73.43.-f
    Quantum Hall effects
  • 03.65.Ud
    Entanglement and quantum nonlocality (e.g. EPR paradox, Bell's inequalities, GHZ states, etc.)
  • 77.22.Ej
    Dielectric polarization and depolarization
  • YEAR: 2006
KEYWORDS: quantum entanglement, Berry phase, entropy, ground states, strongly correlated electron systems, fermion systems

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