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Fair-sampling assumption is not necessary for testing local realism

Source: Phys. Rev. A 81, 012109 (2010); doi:10.1103/PhysRevA.81.012109

Published 13 January 2010

PACS
  • 03.65.Ud
    Entanglement and quantum nonlocality
  • 03.67.-a
    Quantum information
  • 03.65.Ta
    Foundations of quantum mechanics; measurement theory
  • YEAR: 2010
PUBLICATION DATA
Publisher:
AIP is a member of CrossRef APS
Dominic W. Berry,1,2 Hyunseok Jeong,3,4 Magdalena Stobiska,3,5,6 and Timothy C. Ralph3
1Centre for Quantum Computer Technology, Macquarie University, Sydney, NSW 2109, Australia
2Institute for Quantum Computing, University of Waterloo, Waterloo, ON N2L 3G1, Canada
3Centre for Quantum Computer Technology, Department of Physics, The University of Queensland, St Lucia, Qld 4072, Australia
4Center for Subwavelength Optics, Department of Physics and Astronomy, Seoul National University, Seoul, 151-742, Korea
5Institut fr Optik, Information und Photonik, Universitt Erlangen-Nrnberg, Staudtstr. 7/B2, D-91058 Erlangen, Germany
6Institute of Theoretical Physics and Astrophysics, University of Gdask, ul. Wita Stwosza 57, PL-80-952 Gdask, Poland

Almost all Bell inequality experiments to date have used postselection and therefore relied on the fair sampling assumption for their interpretation. The standard form of the fair sampling assumption is that the loss is independent of the measurement settings, so the ensemble of detected systems provides a fair statistical sample of the total ensemble. This is often assumed to be needed to interpret Bell inequality experiments as ruling out hidden-variable theories. Here we show that it is not necessary; the loss can depend on measurement settings, provided the detection efficiency factorizes as a function of the measurement settings and any hidden variable. This condition implies that Tsirelsons bound must be satisfied for entangled states. On the other hand, we show that it is possible for Tsirelsons bound to be violated while the Clauser-Horne-Shimony-Holt (CHSH)-Bell inequality still holds for unentangled states, and present an experimentally feasible example. ©2010 The American Physical Society
History: Received 15 May 2009; revised 8 June 2009; published 13 January 2010
Permalink: http://link.aps.org/abstract/PRA/v81/e012109
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