Undergrad New experimental support for pilot wave theory?

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SUMMARY

The forum discussion centers on the experimental support for the De Broglie-Bohm pilot wave theory, highlighting significant contributions from Howard Wiseman and Lubos Motl. Wiseman emphasizes the importance of terminology in discussing nonlocality, advocating for the distinction between violations of local causality and signal locality. The conversation also critiques the use of weak measurements in experiments related to Bohmian mechanics, asserting that such measurements do not definitively prove the reality of Bohmian trajectories. The discussion references key publications, including the open-access article "Experimental nonlocal and surreal Bohmian trajectories" from *Science Advances*.

PREREQUISITES
  • Understanding of De Broglie-Bohm pilot wave theory
  • Familiarity with Bell's Theorems and nonlocality concepts
  • Knowledge of weak measurements in quantum mechanics
  • Basic grasp of quantum interpretations, including Copenhagen interpretation
NEXT STEPS
  • Read the article "Experimental nonlocal and surreal Bohmian trajectories" in *Science Advances*
  • Explore Howard Wiseman's paper on Bell's Theorems and local causality
  • Investigate the implications of weak measurements in quantum mechanics
  • Study the philosophical implications of realism versus operational interpretations in quantum theory
USEFUL FOR

Physicists, quantum mechanics researchers, and students interested in the foundations of quantum theory, particularly those exploring interpretations of quantum mechanics and the implications of nonlocality.

  • #91
N88 said:
But I was keen to see your "tedious mathematical slog" to learn if you thought non-locality (NL) was anywhere involved. From your other recent comments here, I take it that you (like me) are not in Demystifier's camp when it comes to NL being involved in Bell's (1964) equation (3)? I'm OK with that.
So you don't agree with my post #38? May I know why?
 
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  • #92
N88 said:
In so far as our quantum world is concerned, there is an unrealistic assumption in Bell's (1964) theorem; i.e., the attribution of classicality (via λ) to quantum objects.
But Bell's ##\lambda## is equivalent to my C in post #28. Any yet, you said that my C is OK for you. So you are not being consistent.
 
  • #93
stevendaryl said:
Isn't that what Bell was trying to prove? That QM is inconsistent with certain classical assumptions?

Indeed.

What I don't understand is why he is looking at Bells original paper. Dr Chinese's write up is much simpler:
http://drchinese.com/David/Bell_Theorem_Easy_Math.htm

Once that is understood then you can look at more advanced treatments.

Thanks
Bill
 
  • #94
bhobba said:
What I don't understand is why he is looking at Bells original paper. Dr Chinese's write up is much simpler:
He wants to prove that mainstream understanding is wrong. For that purpose it is much more cool to prove that Bell was wrong than to prove that Dr Chinese is wrong.

Similarly, people who want to prove that theory of relativity is wrong often look at Einstein's original papers. Physicists who accept theory of relativity rarely look at Einstein's original papers.
 
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  • #95
stevendaryl said:
Isn't that what Bell was trying to prove? That QM is inconsistent with certain classical assumptions?
It looks as if some people don't understand the concept of reductio ad absurdum, i.e. making correct conclusion by taking a false assumption.
 
  • #96
I read the elegant paper of Dr Chinese.
Have hidden variables to give outputs to not measured things?
I think that it would be enough if they could predict them for all measurements actually done.
 
  • #97
About P(a,b)=\int d\lambda f(\lambda)P(a,b,\lambda):
Demystifier said:
. The second equation cannot be false, because it is one of the basic general laws in the theory of probability.
Not exactly, it contains the assumption that there is no superdeterminisms. Else, this could be P(a,b)=\int d\lambda f(a,b,\lambda)P(a,b,\lambda)
 
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  • #98
naima said:
Have hidden variables to give outputs to not measured things?
I think that it would be enough if they could predict them for all measurements actually done.
It is, indeed, enough. And in particular dBB theory does not define outputs to not measured things. Except for positions. But for everything else, the "measurement result", even if it is defined in a deterministic way, depends also on the unknown position of the "measurement device". So, without measurement being done there is also no hidden state of the "measurement device", and, therefore, no predicted output.

This property is known as contextuality.
 
  • #99
Ilja said:
About P(a,b)=\int d\lambda f(\lambda)P(a,b,\lambda):

Not exactly, it contains the assumption that there is no superdeterminisms. Else, this could be P(a,b)=\int d\lambda f(a,b,\lambda)P(a,b,\lambda)
Interesting! Is there a reference for that, or is it your own conclusion?
 
  • #100
No, this is my own remark. But it seems quite trivial. That superdeterminism means that the preparation is allowed to know in advance what will be decided by the experimenters is clear. Their decisions what to measure are a and b. Superdeterminism would allow the probability distribution of the hidden variables to depend on a and b. And with this additional possibility you would be unable to proof the theorem.
 
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