OK Corral: Local versus non-local QM

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    Local Qm
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Discussion Overview

The discussion centers around the interpretations of quantum mechanics (QM), specifically the local versus non-local interpretations in the context of the EPR-Bohm experiment involving spin-half particles. Participants explore the implications of these interpretations on the understanding of quantum correlations and the nature of reality as suggested by Bell's theorem.

Discussion Character

  • Debate/contested
  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants argue for a local interpretation of QM, suggesting that the correlations observed in the EPR-Bohm experiment can be explained without invoking non-locality.
  • Others propose that the settings of measuring devices in Bell tests cannot be causally correlated, raising questions about the nature of outcomes and whether they are determined at the point of particle creation or interaction.
  • One participant questions the necessity of the Many-Worlds Interpretation (MWI), suggesting that if outcomes are determined locally, there may be no need for multiple worlds.
  • Another participant discusses the concept of "Alice's world" and "Bob's world," explaining how information is perceived and measured locally, while also addressing the implications of locality in their interactions.
  • Some participants highlight that while interpretations may differ, the mathematical formalism of QM suggests a non-local character, as a single wave function describes multiple particles rather than individual wave functions for each particle.

Areas of Agreement / Disagreement

Participants express differing views on the nature of locality and non-locality in QM. There is no consensus on whether QM is fundamentally local or non-local, and the discussion remains unresolved with multiple competing interpretations being presented.

Contextual Notes

Participants acknowledge the complexity of the interpretations and the mathematical underpinnings of QM, noting that the discussion is constrained to the EPR-Bohm experiment and its implications for understanding quantum correlations.

  • #241
NateTG said:
Applying Occam's Razor to QM produces an 'instrumentalist interpretation' which is explicitly uninterested in anything untestable, and, instead simply predicts probabilities of experimental results. In other words, as long as there are prediction equivalent theories without a physically real wavefunction, Occam's razor tells us there isn't necessarily one.
I disagree. A wavefunction is a much simpler thing than the collection of all humans and their experiments. Occam would tell you to derive the latter from the former (as in MWI) rather than somehow taking it as given.
 
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  • #242
Ontoplankton said:
I disagree. A wavefunction is a much simpler thing than the collection of all humans and their experiments. Occam would tell you to derive the latter from the former (as in MWI) rather than somehow taking it as given.

Well, ultimately, it comes down to what 'simplest' means. And that requires some sort of arbitrary notions.
 
  • #243
I don't know... it's easy to specify a wavefunction; you just write down some equations, and then without any complex further assumptions, you can talk about decoherence and so on to show that humans and their experiments are structures in the wavefunction. But how do you specify the collection of humans and their experiments, without deriving it from something more basic? I think any theory that's anthropocentric like that is bound to violate Occam.
 
  • #244
We have one theory which says that:
1. We can predict experimental results using some method X
2. There are things that are not observable used in X.
3. These unobservable things have physical reality.
And another theory that says:
1. We can predict experimental results using the same method X.
2. There are things that are not observable used in X

Even considering that 'physical reality' is a poorly defined notion, it seems like the latter theory is simpler.
 
  • #245
The crucial difference here being that in the former theory, 1 is explained by 2 and 3, whereas in the latter theory, 1 is an assumption that comes from nowhere. Occam is bothered by complex assumptions, not complex conclusions. Once you've explained something, you can cross it off your list of baggage.

Also, the latter theory isn't complete; either the unobservable things exist or they don't, and you have to pick one.
 
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  • #246
1. We can predict experimental results using QED.
2. The 4-potential A^{\mu} is unobservable.

Surely we don't have to make a choice, but rely on experiment ?
 
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  • #247
Ontoplankton said:
I disagree. A wavefunction is a much simpler thing than the collection of all humans and their experiments. Occam would tell you to derive the latter from the former (as in MWI) rather than somehow taking it as given.
Actually, it is quite possible that you can do without a wavefunction (I guess Occam would be happy):smile: In http://www.arxiv.org/abs/quant-ph/0509044 , the Klein-Gordon-Maxwell electrodynamics is discussed, the unitary gauge is chosen (meaning the wavefunction is real), and it is proven that one can eliminate the wavefunction from the equations and formulate the Cauchy problem for the 4-potential of electromagnetic field. That means that if you know the 4-potential and its time derivatives at some moment in time, you can calculate them for any moment in time, or, in other words, the 4-potential evolves independently.
 

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