Phys. Rev. B 73, 245115 (2006) [10 pages]
Entanglement entropy and the Berry phase in the solid state
Abstract
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Citing Articles
S. RyuKavli Institute for Theoretical Physics, University of California, Santa Barbara, California 93106, USAY. HatsugaiDepartment 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 ×(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
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