Titlebook: Bell‘s Theorem, Quantum Theory and Conceptions of the Universe; Menas Kafatos Book 1989 Springer Science+Business Media B.V. 1989 EPR para

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https://doi.org/10.1007/978-3-030-92968-8n originally considered the case where one could define an “element of reality”, namely for the much simpler case where one could predict with certainty a definite outcome for an experiment For this simple case, Bell’s Theorem says nothing. But by using a slightly more complicated model than Bell, o

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https://doi.org/10.1007/978-3-030-92968-8rner, is interpreted in this paper as the irrelevance of Bell’s inequalities for the problem of local hidden variables in connection with RQFT. This leads to the question how to formulate the problem of local hidden variables in RQFT. By giving a precise definition of hidden theory it is argued that

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Asad Ullah,Shahid Imran,Deena Royc but which violate “causality” as that term is defined by Bell et al. For simple model PDE, I have already shown that certain statistical quantities obey a true Schrodinger equation; in the “non-collapse” view of quantum measurement, this in itself should be enough to reproduce known measurement re

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Vimal K E K,Sonu Rajak,Almoayied Assayedcal hidden-variables model which exactly reproduces the correlation predictions of quantum mechanics in EPRB-type experiments is reported. Its efficiency, symmetry and relation to Caser’s proof are discussed.

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https://doi.org/10.1007/978-3-030-30066-1 comprehension of the experimental results. The example of the singlet state for separate fermions is used to specify the points of contradiction with quantum mechanics, particularly the localization of wave packets and the uncertainty principle. The contradiction between such state and the theory o

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Pinosh Kumar Hajoary,K. B. Akhileshising over the settings on the measurement apparatus, the proof avoids Stapp’s assumption that probabiIities can be equated with relative frequencies. It also avoids the assumption, which Bell and Signer make, that there is a phase-space distribution for which the probabi1ities of quantum theory are

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Peethani Sai Ram,K. Deepak Lawrencee for an antiparticle. The particle amplitude is specified at the initial time and the antiparticle amplitude at the final time. Time reflection invariance indicates that the preparation of the antiparticle state at the final time should be carried out by observers composed of antiparticles. A model

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