Abstract
Harrigan and Spekkens (Found Phys 40:125–157, 2010), introduced the influential notion of an ontological model of operational quantum theory. Ontological models can be either “epistemic” or “ontic.” According to the two scholars, Einstein would have been one of the first to propose an epistemic interpretation of quantum mechanics. Pusey et al. (Nat Phys 8:475–478, 2012) showed that an epistemic interpretation of quantum theory is impossible, so implying that Einstein had been refuted. We discuss in detail Einstein’s arguments against the standard interpretation of QM, proving that there is a misunderstanding in Harrigan and Spekkens’ attribution of an epistemic perspective to Einstein, whose point of view was actually statistical, but in a quasi-classical sense.
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Notes
But see footnote 15.
Note that the common opinion is that quantum mechanics violates S but not LC; see, for instance, the papers collected in Cushing and McMullin (1989).
Obviously, Einstein’s strong completeness presupposes EPR’s one, in the sense that if one or more elements of reality would not be represented in the theory, the bijective correspondence would not exist.
According to Howard (2015, pp. 128ff.), Einstein was progressively aware of the distinction between locality and separability. Here, we will not insist on this distinction.
It should be noted, however, that some scholars find controversial and dubious the foundational significance of PBR’s assumptions. For instance, Mansfield (2016) does not agree on the acceptability of “preparation independence” as a premise of PBR’s argument.
Perhaps PBR is a threat for QBism. Indeed, Fuchs and Schack (2015), in order to avoid problems for QBism deriving from PBR’s argument, deny that QBism is an ontological model in HS’ sense.
Just an example: We know that light is a wave phenomenon. However, the first models of its behavior were couched in the framework of geometrical optics. This theory is, thus, an epistemically incomplete theory insofar as it does not capture the undulatory aspects of light; it does not allow for reaching full knowledge of this physical phenomenon. Nevertheless, geometrical optics is not ontologically incomplete with respect to the wave character of light, since, intrinsically, it does not possess the theoretical ingredients able to describe electromagnetic waves. Both an epistemically incomplete theory and an ontologically incomplete one are not the best theories to capture a certain class of phenomena, but the former cannot even be the best theory as, being, as it were, at the maximum of its possibilities, it is not able to take into account some phenomena, so that it is condemned to remain incomplete. The latter actually could be the best theory, in the sense that, not having fully exploited its potentialities, it could be made complete, at least in principle.
It is also HS’ completeness.
Note that if separability does not hold, it would not be possible to introduce separated wave functions as ψ1 and ψ2.
Lehner (2014, pp. 331ff.) interprets Einstein’s argument in the same way. Nonetheless, he emphasizes that the jump from the many terms of the theory for one reality to one term for many realities does not hold. But Einstein (both in dialectica and in Schilpp’s volume) begins his argument assuming only two possible positions: the standard one and the incompleteness one. The former presupposes a 1-1 relation between theory and reality. Therefore, after showing that this does not hold (provided the acceptance of separability and locality), one is compelled to endorse the other attitude. Moreover, the many wave functions connected to different measurements represent different aspects of the physical reality of system B, so that the generic ψAB preceding the measurement is statistically incomplete.
The standard answer to Einstein’s argument would be that it is sufficient to give up separability—a possibility Einstein never accepted—to avoid the multiple wave functions; and the violation of separability is not incompatible with relativity.
That is, these particles follow Maxwell–Boltzmann statistics.
Note that, using HS’ language, a statistical interpretation states that p2(k/l1,M)p2(k/l2,M) ≠ 0, with l1 and l2 ∈ Λ and l1 ≠ l2. It is not obvious that this implies p1(λ|Pψ)p1(λ|Pφ) ≠ 0. In other terms, even if the same measurement, given different situations, could produce the same outcome, this does not entail (prima face) that two different preparations produce the same ontic situation.
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We thank Claudio Calosi, who discussed with us the topic of the paper.
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Fano, V., Macchia, G. & Tarozzi, G. Is Einstein’s Interpretation of Quantum Mechanics Ψ-Epistemic?. Axiomathes 29, 607–619 (2019). https://doi.org/10.1007/s10516-018-9382-6
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DOI: https://doi.org/10.1007/s10516-018-9382-6