Count Iblis
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http://arxiv.org/abs/0902.3376"
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The discussion revolves around Hardy's Paradox and its implications for various interpretations of quantum mechanics (QM), particularly focusing on Lorentz invariance and the compatibility of different theories with relativistic frameworks. Participants explore theoretical implications, challenges, and potential resolutions related to the paradox.
Participants express differing views on the compatibility of various interpretations of quantum mechanics with Lorentz invariance, and there is no consensus on the viability of Towler's proposal or the implications of the discussed papers. The discussion remains unresolved with multiple competing perspectives.
Limitations include the dependence on specific interpretations of quantum mechanics and the unresolved nature of the mathematical steps involved in the proposed theories. The discussion also highlights the complexity of reconciling different theoretical frameworks.
Count Iblis said:http://arxiv.org/abs/0902.3376"
Yes, he is saying that. But he was not aware ofDrChinese said:he is saying ... Bohmian mechanics have problems with achieving Lorentz invariance
Demystifier said:Yes, he is saying that. But he was not aware of
http://xxx.lanl.gov/abs/0811.1905 [accepted for publication in Int. J. Quantum Inf.]
which, I believe, solves these problems. (When I saw Marchildon's paper few days ago, I have sent him a note regarding the paper above and he seemed to be interested about it. Maybe he will take it into account in a revised version of his paper.)
It certainly is a viable option, even in curved spacetime (needed by general relativity). Nevertheless, such a version certainly looses some of its mathematical elegance. (The mathematical elegance is one of the reasons why I become interested in non-relativistic Bohmian mechanics in the first place.) If Bohmian mechanics is hoped to be a fundamental theory, then it is natural to require the mathematical elegance. For that reason, I prefer searching for a completely relativistic-covariant formulation. For the case in which particle creation can be neglected, the paper I mentioned above completely achieves that goal. Moreover, it provides a simple counterexample to various "theorems" claiming that relativistic-covariant nonlocal hidden variable theory is impossible. The crucial "new" idea in this paper that makes Lorentz covariance possible is the observation that |psi|^2 is not a probability density in space, but in SPACETIME. Such an idea may look as a deviation from experimentally confirmed probabilistic interpretation of psi, but, as explained in the paper, this idea is in a complete agreement with experiments.DrChinese said:I saw some interesting stuff following Towler's http://www.tcm.phy.cam.ac.uk/~mdt26/pilot_waves.html. He was saying that the Lorentz version of space-time should be kept, and the Einstein version of SR should be dropped. He says that makes things play nicer with Pilot Wave (BM/dBB) theory and perhaps solves some of the issues. I had not heard such a strong perspective on the matter before. Is this a viable option? I would guess that it would run afoul of General Relativity pretty quickly. Although I guess the Lorentz version of spacetime would have a lot of similarities with SR and therefore GR anyway.