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Phys. Rev. A 73, 066102 (2006) [1 pages]

Reply to "Comment on `All quantum observables in a hidden-variable model must commute simultaneously'" [Phys. Rev. A 73, 066101 (2006)]

J. D. Malley1 and A. Fine2
1Center for Information Technology, NIH, Bethesda, Maryland 20892, USA
2Department of Philosophy, University of Washington, Seattle, Washington 98195, USA

Received 10 March 2006; published 14 June 2006

Nagata [Phys. Rev. A 73, 066101 (2006)] questions whether a general no-go theorem of Malley [Phys. Rev. A 69, 022118 (2004)] applies to local hidden variables and outlines a "counterexample." In fact this is not a counterexample at all, but in seeing why it fails we clarify the significance of Malley's result and its relation to other no-go theorems.

©2006 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevA.73.066102
DOI: 10.1103/PhysRevA.73.066102
PACS: 03.65.Ca; 03.65.Ud
  • 03.65.Ca
    Formalism in quantum mechanics
  • 03.65.Ud
    Entanglement and quantum nonlocality (e.g. EPR paradox, Bell's inequalities, GHZ states, etc.)
  • YEAR: 2006
KEYWORDS: quantum theory

See Also

Comment on "All quantum observables in a hidden-variable model must commute simultaneously"
Koji Nagata
Phys. Rev. A 73, 066101 (2006)

All quantum observables in a hidden-variable model must commute simultaneously
James D. Malley
Phys. Rev. A 69, 022118 (2004)

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Related Articles

  1. Comment on "All quantum observables in a hidden-variable model must commute simultaneously"
    Koji Nagata
    Phys. Rev. A 73, 066101 (2006)
  2. All quantum observables in a hidden-variable model must commute simultaneously
    James D. Malley
    Phys. Rev. A 69, 022118 (2004)


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