Abstract
Contextuality and nonlocality (hence nonobjectivity of physical properties) are usually maintained to be unavoidable features of quantum mechanics (QM), following from its mathematical apparatus. Moreover they are considered as basic in quantum information processing. Nevertheless they raise still unsolved problems, as the objectification problem in the quantum theory of measurement. The extended semantic realism (ESR) model offers a way out from these difficulties by reinterpreting quantum probabilities as conditional rather than absolute and embedding the mathematical formalism of QM into a broader mathematical framework. A noncontextual hidden variables theory can then be constructed which justifies the assumptions introduced in the ESR model and proves its objectivity. Both linear and nonlinear time evolution occur in this model, depending on the physical environment, as in QM. In addition, the ESR model implies modified Bell’s inequalities that do not necessarily conflict with QM, supplies different mathematical representations of proper and improper mixtures, provides a general framework in which the local interpretations of the GHZ experiment obtained by other authors are recovered, and supports an interpretation of quantum logic which avoids the introduction of the problematic notion of quantum truth.
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It must be noted that the term “realistic” is used here in a very weak sense. Well known interpretations or modifications of QM, as Bohm’s theory, multi-world interpretations and GRW theory, are “realistic” in a much stronger sense and will not be considered in this paper.
An intuitive explanation of this result can be given as follows: the detection probabilities change with the measurement that is performed, and the subset of individual objects that is detected generally is not a fair sample of the set of all objects that are produced. This argument resembles the argument that has been often raised to question the results of Aspect’s and similar experiments, in which fair sampling is usually assumed [20, 21]. But unfair sampling depends on the features of real measuring devices in the latter argument: hence it would not occur in the case of idealized measurements. It depends instead on the physical properties of the individual objects, hence on different physical variables, in the ESR model, so that it may occur also in the case of idealized measurements [22]. We add that the conventional interpretation of the “no-go” theorems has been questioned in particular by several authors in the framework of a statistical interpretation of QM that maintains the standard interpretation of quantum probabilities [23–27]. The criticism of this “statistical opposition” leads to avoid nonlocality of QM, while contextuality is preserved and explained, in the case of photons, by taking into account the thresholds that occur in real detectors [28, 29]. Our present view is obviously different, for it refers to a “realistic” interpretation of QM and circumvents the “no-go” theorems by modifying the standard interpretation of quantum probabilities, thus avoiding contextuality, hence nonlocality.
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Garola, C. A Survey of the ESR Model for an Objective Reinterpretation of Quantum Mechanics. Int J Theor Phys 54, 4410–4422 (2015). https://doi.org/10.1007/s10773-015-2618-y
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DOI: https://doi.org/10.1007/s10773-015-2618-y