scholarly journals Does particle decay cause wave function collapse: an experimental test

2003 ◽  
Vol 308 (5-6) ◽  
pp. 323-328 ◽  
Author(s):  
Spencer R. Klein ◽  
Joakim Nystrand
2018 ◽  
Vol 426 ◽  
pp. 212-218
Author(s):  
R.S.N. Moreira ◽  
A.J.A. Carvalho ◽  
M.S. Mendes ◽  
M.G.M. Moreno ◽  
J. Ferraz ◽  
...  

Author(s):  
R. S. N. Moreira ◽  
A. J. A. Carvalho ◽  
J. Ferraz ◽  
F. Parisio ◽  
L. H. Acioli ◽  
...  

2015 ◽  
Vol 56 (8) ◽  
pp. 082103
Author(s):  
Charles Wesley Cowan ◽  
Roderich Tumulka

2018 ◽  
Vol 2018 ◽  
pp. 1-13
Author(s):  
Antonio Accioly ◽  
Wallace Herdy

The equivalence principle (EP) and Schiff’s conjecture are discussed en passant, and the connection between the EP and quantum mechanics is then briefly analyzed. Two semiclassical violations of the classical equivalence principle (CEP) but not of the weak one (WEP), i.e., Greenberger gravitational Bohr atom and the tree-level scattering of different quantum particles by an external weak higher-order gravitational field, are thoroughly investigated afterwards. Next, two quantum examples of systems that agree with the WEP but not with the CEP, namely, COW experiment and free fall in a constant gravitational field of a massive object described by its wave-function Ψ, are discussed in detail. Keeping in mind that, among the four examples focused on in this work only COW experiment is based on an experimental test, some important details related to it are presented as well.


2020 ◽  
Vol 18 ◽  
pp. 129-153
Author(s):  
Jeffrey Boyd

In Quantum ElectroDynamics (QED) the propagator is a function that describes the probability amplitude of a particle going from point A to B. It summarizes the many paths of Feynman’s path integral approach. We propose a reverse propagator (R-propagator) that, prior to the particle’s emission, summarizes every possible path from B to A. Wave function collapse occurs at point A when the particle randomly chooses one and only one of many incident paths to follow backwards with a probability of one, so it inevitably strikes detector B. The propagator and R-propagator both calculate the same probability amplitude. The R-propagator has an advantage over the propagator because it solves a contradiction inside QED, namely QED says a particle must take EVERY path from A to B. With our model the particle only takes one path. The R-propagator had already taken every path into account. We propose that this tiny, infinitesimal change from propagator to R-propagator would vastly simplify the mathematics of Nature. Many experiments that currently describe the quantum world as weird, change their meaning and no longer say that. The quantum world looks and acts like the classical world of everyday experience.


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