Home | About Journal | Web Links | E-mail Alerts | RSS RSS Icon | Browse
Previous Article Next Article

Maximally entangled three-qubit states via geometric measure of entanglement

Source: Phys. Rev. A 80, 052315 (2009); doi:10.1103/PhysRevA.80.052315

Published 11 November 2009

KEYWORDS and PACS
Keywords
PACS
  • 03.67.Mn
    Entanglement measures, witnesses, and other characterizations (quantum information)
  • 03.65.Ud
    Entanglement and quantum nonlocality
  • YEAR: 2009
PUBLICATION DATA
Publisher:
AIP is a member of CrossRef APS
Sayatnova Tamaryan
Theory Department, Yerevan Physics Institute, Yerevan 375036, Armenia

Tzu-Chieh Wei
Institute for Quantum Computing and Department of Physics and Astronomy, University of Waterloo, Waterloo, Ontario, Canada and Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia, Canada

DaeKil Park
Department of Physics, Kyungnam University, Masan 631-701, Korea
Bipartite maximally entangled states have the property that the largest Schmidt coefficient reaches its lower bound. However, for multipartite states, the standard Schmidt decomposition generally does not exist. We use a generalized Schmidt decomposition and the geometric measure of entanglement to characterize three-qubit pure states and derive a single-parameter family of maximally entangled three-qubit states. The paradigmatic Greenberger-Horne-Zeilinger (GHZ) and W states emerge as extreme members in this family of maximally entangled states. This family of states possesses different trends of entanglement behavior: in going from GHZ to W states, the geometric measure, the relative entropy of entanglement, and the bipartite entanglement all increase monotonically whereas the three-tangle and bipartition negativity both decrease monotonically. ©2009 The American Physical Society
History: Received 27 May 2009; published 11 November 2009
Permalink: http://link.aps.org/abstract/PRA/v80/e052315
ADVERTISEMENT