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Foundations of Physics Letters

Basic Neutron Interference Experiments and the Information Interpretation of the Wavefunction

Michael Zawisky

Published Nov 1, 2004• 5 citations
Publisher
DOI
10.1007/s10702-004-0904-7

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The basic postulates The statistical interpretation of the wavefunction is in accord with experimental facts. An interference pattern on a screen is built up by a series of apparently random events, and the wavefunction correctly predicts where the particle is most likely to land over an ensemble of trials (cf. the frontispiece ). Yet the interpretation of the wavefunction which ascribes to it a purely statistical significance is not forced on us by the experimental results – the latter show only that it is consistent to regard the wavefunction as containing information on probability; they do not exclude the possibility that it may possess other properties. On the contrary, one may take the view that the characteristic distribution of spots on a screen which build up an interference pattern is evidence that the wavefunction indeed has a more potent physical role than a mere repository of information on probabilities, for how are the particles guided so that statistically they fall into such a pattern? Such a question is naturally ruled out by the purely probabilistic interpretation. But the latter is appropriate only if we wish to reduce physics to a kind of algorithm which is efficient at correlating the statistical results of experiments. If we wish to do more, and attempt to understand the experimental results as the outcome of a causally connected series of individual processes, then we are free to enquire as to the possible further significance of the wavefunction (beyond its probabilistic aspect), and to introduce other concepts in addition to the wavefunction.

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The basic postulates The statistical interpretation of the wavefunction is in accord with experimental facts. An interference pattern on a screen is built up by a series of apparently random events, and the wavefunction correctly predicts where the particle is most likely to land over an ensemble of trials (cf. the frontispiece ). Yet the interpretation of the wavefunction which ascribes to it a purely statistical significance is not forced on us by the experimental results – the latter show only that it is consistent to regard the wavefunction as containing information on probability; they do not exclude the possibility that it may possess other properties. On the contrary, one may take the view that the characteristic distribution of spots on a screen which build up an interference pattern is evidence that the wavefunction indeed has a more potent physical role than a mere repository of information on probabilities, for how are the particles guided so that statistically they fall into such a pattern? Such a question is naturally ruled out by the purely probabilistic interpretation. But the latter is appropriate only if we wish to reduce physics to a kind of algorithm which is efficient at correlating the statistical results of experiments. If we wish to do more, and attempt to understand the experimental results as the outcome of a causally connected series of individual processes, then we are free to enquire as to the possible further significance of the wavefunction (beyond its probabilistic aspect), and to introduce other concepts in addition to the wavefunction.
Abstract The conventional theory of non-relativistic neutron beam scattering from many-body systems treats the beam essentially as a classical system, because the neutron dynamical variables are captured in the main theoretical formulas (e.g. time-correlation functions) not as quantum mechanical operators but as c-numbers only. This simplification results in the full decoupling of the probe particles’ dynamics from the quantum dynamics of the scatterer. Further, neutrons’ wavefunctions are represented with plane waves, and thus the concept of neutron’s finite coherence length in momentum space becomes irrelevant. Making contact with modern quantum theoretical approaches (e.g., quantum entanglement, Feynman paths, “which-path information” versus interference, Weak Values theory) new observable effects of non-relativistic quantum beam scattering may be exposed and/or predicted, such as a surprising intensity deficit in neutron Compton scattering (NCS) of epithermal neutrons from protons of H-containing materials. Here, the NCS-intensity deficit observed in scattering from liquid C6H6 is discussed and interpreted from first principles, in the general frame of Weak Values theory. Moreover, based on Feynman’s didactical argument that there isn’t any interference between distinguishable neutron paths, we show that this NCS-effect cannot be interpreted as being caused by destructive interference of neutron paths scattered from entangled (two or a few) protons, as was earlier proposed by some authors.