{ "id": "cond-mat/0601237", "version": "v3", "published": "2006-01-11T18:51:07.000Z", "updated": "2006-05-17T01:44:04.000Z", "title": "Entanglement entropy and the Berry phase in solid states", "authors": [ "S. Ryu", "Y. Hatsugai" ], "comment": "11 pages, 4 figures, new references added", "journal": "Phys. Rev. B 73, 245115 (2006)", "doi": "10.1103/PhysRevB.73.245115", "categories": [ "cond-mat.mes-hall", "cond-mat.str-el", "quant-ph" ], "abstract": "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 $\\pi \\times ({odd integer})$ 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 this lower bound is related to vanishing of the expectation value of a certain non-local operator which creates a kink in 1D systems.", "revisions": [ { "version": "v3", "updated": "2006-05-17T01:44:04.000Z" } ], "analyses": { "keywords": [ "entanglement entropy", "berry phase", "solid states", "ground state", "von neumann entropy" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. B" }, "note": { "typesetting": "TeX", "pages": 11, "language": "en", "license": "arXiv", "status": "editable" } } }