Why interference phenomena do not capture the essence of quantum theory

Author:

Catani Lorenzo1,Leifer Matthew2,Schmid David3,Spekkens Robert W.4

Affiliation:

1. Electrical Engineering and Computer Science Department, Technische Universität Berlin, 10587 Berlin, Germany

2. Institute for Quantum Studies and Schmid College of Science and Technology, Chapman University, One University Drive, Orange, CA, 92866, USA

3. International Centre for Theory of Quantum Technologies, University of Gdansk, 80-308 Gdansk, Poland

4. Perimeter Institute for Theoretical Physics, 31 Caroline Street North, Waterloo, Ontario Canada N2L 2Y5

Abstract

Quantum interference phenomena are widely viewed as posing a challenge to the classical worldview. Feynman even went so far as to proclaim that they are the only mystery and the basic peculiarity of quantum mechanics. Many have also argued that basic interference phenomena force us to accept a number of radical interpretational conclusions, including: that a photon is neither a particle nor a wave but rather a Jekyll-and-Hyde sort of entity that toggles between the two possibilities, that reality is observer-dependent, and that systems either do not have properties prior to measurements or else have properties that are subject to nonlocal or backwards-in-time causal influences. In this work, we show that such conclusions are not, in fact, forced on us by basic interference phenomena. We do so by describing an alternative to quantum theory, a statistical theory of a classical discrete field (the `toy field theory') that reproduces the relevant phenomenology of quantum interference while rejecting these radical interpretational claims. It also reproduces a number of related interference experiments that are thought to support these interpretational claims, such as the Elitzur-Vaidman bomb tester, Wheeler's delayed-choice experiment, and the quantum eraser experiment. The systems in the toy field theory are field modes, each of which possesses, at all times, both a particle-like property (a discrete occupation number) and a wave-like property (a discrete phase). Although these two properties are jointly possessed, the theory stipulates that they cannot be jointly known. The phenomenology that is generally cited in favour of nonlocal or backwards-in-time causal influences ends up being explained in terms of inferences about distant or past systems, and all that is observer-dependent is the observer's knowledge of reality, not reality itself.

Funder

Perimeter Institute

Publisher

Verein zur Forderung des Open Access Publizierens in den Quantenwissenschaften

Subject

Physics and Astronomy (miscellaneous),Atomic and Molecular Physics, and Optics

Reference109 articles.

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2. Niels Bohr. Discussion with einstein on epistemological problems in atomic physics. In Paul Arthur Schilpp, editor, The Library of Living Philosophers, Volume 7. Albert Einstein: Philosopher-Scientist, pages 199–241. Open Court, 1949. URL: https://philpapers.org/rec/BOHDWE.

3. Stephen D. Bartlett, Terry Rudolph, and Robert W. Spekkens. Reconstruction of gaussian quantum mechanics from liouville mechanics with an epistemic restriction. Phys. Rev. A, 86:012103, Jul 2012. doi:https://doi.org/10.1103/PhysRevA.86.012103.

4. Avshalom C. Elitzur and Lev Vaidman. Quantum mechanical interaction-free measurements. Found. Phys., 23(7):987–997, Jul 1993. doi:https://doi.org/10.1007/BF00736012.

5. John Archibald Wheeler. The ``past'' and the ``delayed-choice'' double-slit experiment. In A.R. Marlow, editor, Mathematical Foundations of Quantum Theory, pages 9–48. Academic Press, 1978. doi:https://doi.org/10.1016/B978-0-12-473250-6.50006-6.

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