David Bourget (Western Ontario)
David Chalmers (ANU, NYU)
Rafael De Clercq
Ezio Di Nucci
Jonathan Jenkins Ichikawa
Jack Alan Reynolds
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Foundations of Physics 36 (10):1573-1586 (2006)
It is known that the global state of a composite quantum system can be completely determined by specifying correlations between measurements performed on subsystems only. Despite the fact that the quantum correlations thus suffice to reconstruct the quantum state, we show, using a Bell inequality argument, that they cannot be regarded as objective local properties of the composite system in question. It is well known since the work of Bell, that one cannot have locally preexistent values for all physical quantities, whether they are deterministic or stochastic. The Bell inequality argument we present here shows this is also impossible for correlations among subsystems of an individual isolated composite system. Neither of them can be used to build up a world consisting of some local realistic structure. As a corrolary to the result we argue that entanglement cannot be considered ontologically robust. The Bell inequality argument has an important advantage over others because it does not need perfect correlations but only statistical correlations. It can therefore easily be tested in currently feasible experiments using four particle entanglement
|Keywords||ontology quantum correlations Bell inequality entanglement|
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References found in this work BETA
J. S. Bell (2004 ). On the Einstein-Podolsky-Rosen Paradox. In Speakable and Unspeakable in Quantum Mechanics. Cambridge University Press 14--21.
Simon Kochen & E. P. Specker (1967). The Problem of Hidden Variables in Quantum Mechanics. Journal of Mathematics and Mechanics 17:59--87.
David Mermin (1998). What is Quantum Mechanics Trying to Tell Us? American Journal of Physics 66 (9):753-767.
Citations of this work BETA
Matteo Morganti (2009). A New Look at Relational Holism in Quantum Mechanics. Philosophy of Science 76 (5):1027--1038.
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