Bell's theorem, QFT, and the Relativity of Simultaneity

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Discussion Overview

The discussion revolves around the application of the relativity of simultaneity in quantum field theory (QFT) and its implications for the outcomes of Bell tests. Participants explore the conceptual challenges posed by these ideas through thought experiments involving observers in relative motion, specifically focusing on the Stern Gerlach experiment.

Discussion Character

  • Exploratory
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant describes a thought experiment involving Alice and Bob, where the relativity of simultaneity leads to different perceptions of events occurring at the same time in different frames of reference.
  • Questions are raised about whether events that are simultaneous in one frame remain non-simultaneous in a relatively moving frame, with a participant expressing certainty about this point but seeking clarification.
  • Another participant asserts that the statement "has already happened" in one frame has no physical significance and is coordinate dependent, suggesting that this affects the interpretation of causal links in Bell's theorem.
  • A participant expresses confusion about the physical implications of simultaneity and causality in the context of the Stern Gerlach experiment, questioning the significance of events being actualized in different reference frames.
  • There is an exploration of the idea that the outcome of the Stern Gerlach run may be considered an observable phenomenon in Alice's frame prior to her passing Bob, while it remains unactualized in Bob's frame.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the implications of the relativity of simultaneity for the outcomes of quantum experiments. Multiple competing views regarding the physical significance of simultaneity and causality remain present in the discussion.

Contextual Notes

Participants express varying levels of understanding regarding the mathematical and conceptual frameworks of QFT and relativity, indicating potential limitations in their interpretations and the need for further clarification on these complex topics.

  • #61
DrChinese said:
On the other hand, dBB is a viable interpretation of QM that lacks classical causality despite what you say. Obviously, there are FTL effects present which remove what is usually considered the classical element. Not sure why you would claim otherwise. The whole point of dBB is that its non-locality is manifest.
No. There is no lack of classical causality in dBB. There is no Einstein locality in dBB, but classical causality in a preferred frame.
 
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  • #62
Elias1960 said:
classical causality

What is your definition of "classical causality"?
 
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  • #63
Elias1960 said:
No. There is no lack of classical causality in dBB. There is no Einstein locality in dBB, but classical causality in a preferred frame.

When an action here affects an outcome there (and vice versa), that is not "classical causality" in my book since it is quite obviously the "out" needed a la Bell. It is causal/deterministic, as you say, and locality fails. To use Bell's words, it has a "grossly nonlocal structure". I won't even begin to discuss the issue of preferred frames in dBB, as that is entirely different discussion and belongs in a different thread.

At this point we are arguing about the definition of a word ("classical"), and I doubt we gain anything from tripping down that path.
 
  • #64
PeterDonis said:
What is your definition of "classical causality"?
Causality as used in classical, pre-relativistic physics. Where Newtonian mechanics, despite its action at a distance, is nonetheless considered causal. The cause has to precede the effect in Newtonian absolute time. Reichenbach's common cause principle holds.
DrChinese said:
When an action here affects an outcome there (and vice versa), that is not "classical causality" in my book since it is quite obviously the "out" needed a la Bell. It is causal/deterministic, as you say, and locality fails. To use Bell's words, it has a "grossly nonlocal structure". I won't even begin to discuss the issue of preferred frames in dBB, as that is entirely different discussion and belongs in a different thread.

At this point we are arguing about the definition of a word ("classical"), and I doubt we gain anything from tripping down that path.
The first sentence simply does not make sense to me. I don't see any issue of a preferred frame in dBB, it is quite obvious that if a preferred frame is allowed, dBB can be defined so that it will be causal, deterministic and nonlocal in the absolute time of the preferred frame.

So I don't understand the problems you have with the notion of classical causality, simply because I don't see any different notions of classical causality which could be confused.
 
  • #65
Elias1960 said:
Causality as used in classical, pre-relativistic physics.

Ok, that makes your position clearer.

Elias1960 said:
I don't see any different notions of classical causality which could be confused.

The term "classical" is often used to include relativity. Those who prefer such usage (which includes me) will certainly have a different notion of "classical causality" from yours, since in relativity causality is limited to within the light cone.
 
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