Necessity of Bell's experiment

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Discussion Overview

The discussion revolves around the necessity of Bell's experiment in proving the absence of local hidden variables in quantum mechanics. Participants explore the implications of determinism, the role of initial conditions in experiments, and the significance of Bell's inequalities in the context of quantum correlations and local causality.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • Some participants argue that any experiment with the same initial conditions yielding different results indicates a lack of determinism, questioning the need for Bell's experiment.
  • Others suggest that stochastic theories imply that one cannot fully control or know all initial conditions, allowing for apparent indeterminism even in deterministic frameworks.
  • A participant highlights that Bell's theorem demonstrates the incompatibility of local hidden variables with quantum mechanics, emphasizing the significance of local causality.
  • Some contributions mention that Bell's inequalities may not be necessary to rule out locality for certain theories, suggesting that simpler arguments could suffice.
  • One participant presents a calculation comparing quantum and classical probabilities of entangled particles, asserting that the results demonstrate incompatibility between local hidden variable theories and quantum mechanics.
  • Another participant notes that the discussion should focus on "spooky action at a distance" rather than determinism, referencing Bell's views on local causality.

Areas of Agreement / Disagreement

Participants express differing views on the necessity and implications of Bell's experiment, with no consensus reached on whether Bell's inequalities are essential for ruling out local hidden variables or if simpler arguments could suffice.

Contextual Notes

Some participants mention limitations in controlling all initial conditions due to the complexity of experimental setups, which may affect the interpretation of determinism and indeterminism in quantum mechanics.

guillefix
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Hello, I was just wondering why do you need Bell's experiment to prove that there are no local hidden variables? If you do ANY experiment with the same initial conditions, and you don't get the same result, then it's clear the universe is not deterministic! is it not?

I guess you can say, how can you control the whole universe? But if you create a photon, then you just need to control the past light cone since the photon was created, which is considerably much easier.

I guess then tha Bohms theory suggest that what causes things to look underteminsitic is things outside this cone affecting the result.

Anyway, my question is that if any experiment would be valid for proving this, why is Bell's experiment all that important?

It seems to me that Bell's inequality experiment is just proving that the particles are correlated because the inequality assumes the particles are random (doesnt matter wether statistically or fundamentally) but uncorrelated, and thus it will be violated by particles that are correlated.
 
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guillefix said:
Hello, I was just wondering why do you need Bell's experiment to prove that there are no local hidden variables? If you do ANY experiment with the same initial conditions, and you don't get the same result, then it's clear the universe is not deterministic! is it not?

There are stochastic type theories which postulate that you do not have access to sufficient information to prepare the initial conditions in the manner you describe. Therefore there is apparent indeterminism even though the underlying physical processes are purely deterministic. Bell demonstrates this is not possible for local physical operations, or more accurately, is incompatible with quantum mechanics.
 
guillefix said:
If you do ANY experiment with the same initial conditions, and you don't get the same result, then it's clear the universe is not deterministic! is it not?
It is not. The problem is that you can never know that ALL the initial conditions were the same. A typical experimental apparatus has at least 10^23 degrees of freedom, while you can really control only a few of them. Considering only the past light cone does not change this fact significantly.
 
DrChinese said:
There are stochastic type theories which postulate that you do not have access to sufficient information to prepare the initial conditions in the manner you describe. Therefore there is apparent indeterminism even though the underlying physical processes are purely deterministic. Bell demonstrates this is not possible for local physical operations, or more accurately, is incompatible with quantum mechanics.

Is the main difference that in QM there's always half probability of going through with entangled photons no matter the polarization, but as in classical M photons have a certain polarization the probability depends? Anyway i can't see how they would yield different results. Probably that was the genius of Bell

Btw sorry for answering late
 
guillefix said:
Hello, I was just wondering why do you need Bell's to prove that there are no local hidden variables? If you do ANY experiment with the same initial conditions, and you don't get the same result, then it's clear the universe is not deterministic! is it not?

to that respect

http://www.springerlink.com/content/h105488q281v42p4/fulltext.pdf

...Finally, our results demonstrate that one doesn’t need the “big guns” of Bell’s theorem to rule out locality for any theories in which ψ is given ontic status; more straightforward arguments suffice. Bell’s argument is only necessary to rule out locality for ψ-epistemic hidden variable theories...
 
guillefix said:
Hello, I was just wondering why do you need Bell's experiment to prove that there are no local hidden variables? If you do ANY experiment with the same initial conditions, and you don't get the same result, then it's clear the universe is not deterministic! is it not?

I guess you can say, how can you control the whole universe? But if you create a photon, then you just need to control the past light cone since the photon was created, which is considerably much easier.

I guess then tha Bohms theory suggest that what causes things to look underteminsitic is things outside this cone affecting the result.

Anyway, my question is that if any experiment would be valid for proving this, why is Bell's experiment all that important?

It seems to me that Bell's inequality experiment is just proving that the particles are correlated because the inequality assumes the particles are random (doesnt matter wether statistically or fundamentally) but uncorrelated, and thus it will be violated by particles that are correlated.
You cannot know that the initial conditions are the same if you don't know if there are no hidden variables. :wink: Moreover, you seem to think that the main issue is determinism. It's not. Instead, it's about what seems to be, as Einstein called it, "spooky action at a distance".

Bell: "What is held sacred is the principle of "local causality" or "no action at a distance". [..] It is remarkably difficult to get this point across, that determinism is not the presupposition of the analysis. There is a widespread and erroneous conviction that for Einstein determinism was always the sacred principle."
- cdsweb.cern.ch/record/142461/files/198009299.pdf
 
Ok, I get it. Local hidden variables won't give the same result as quantum mechanics, so it's a no-go theorem. I wanted to check this and I calculated the probability of the spin of one of two entangled electrons being up along z, and the other up along 1/sqrt(2)*z+1/sqrt(2)*x, and got 0.07322, and then did a classical case in which electrons have certain correlated spins but randomlly distributed, and got 0.36254. So if my working is right, this proves they are incompatible!
 
guillefix said:
Hello, I was wondering why do you Bell's to prove that there are no local variables?


...It is important to comment on some of the facts that are commonly overlooked in obtaining the conclusion that quantum theory violates local causality. Firstly, not needed are Bell’s inequalities . Secondly, not needed is a ‘free will’ assumption whereby one assumes a form of
independence between λ and the settings a, b. Thirdly, there is no need for an analysis of the ‘collapse of the wavefunction’ as a real physical process...

http://arxiv.org/pdf/1010.3714v1
 

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