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The Western Ontario series in philosophy of science

Locality and Lorentz-Covariance in the Modal Interpretation of Quantum Mechanics

Dennis Dieks

Published Jan 1, 1998• 6 citations
Publisher
DOI
10.1007/978-94-011-5084-2_3

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In relativistic quantum field theory the notion of a local operation is regarded as basic: each open space-time region is associated with an algebra of observables representing possible measurements performed within this region. It is much more difficult to accommodate the notions of events taking place in such regions or of localized objects. But how can the notion of a local operation be basic in the theory if this same theory would not be able to represent localized measuring devices and localized events? After briefly reviewing these difficulties we discuss a strategy for eliminating the tension, namely by interpreting quantum theory in a realist way. To implement this strategy we use the ideas of the modal interpretation of quantum mechanics. We then consider the question of whether the resulting scheme can be made Lorentz invariant.
Abstract Although Bell’s theorem tells us that any interpretation of quantum mechanics must fail to satisfy Bell’s locality condition, the question of Lorentz­invariance is apparently left open by Bell’s theorem. In­ deed, it has been argued by many that nonlocality is compatible with Lorentz­invariance, given certain interpretations of the latter, or of the former. Some give a ‘weak’ interpretation of Lorentz­ invariance, compatible with a ‘strong’ violation of locality. For example, Bohm’s (1952) theory violates locality in a way that requires a preferred frame; but empirical Lorentz­invariance is preserved in the Bohm theory ­ there is no experiment that could determine the preferred frame. (See, for example, Valentini (199la,b), Bohm and Hiley (1993), and Cushing (1994).) On the other hand, ‘orthodox’ interpretations of special relativity maintain a notion of ‘fundamental