Quantum mechanics is not weird, unless presented as such

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Discussion Overview

The discussion revolves around the nature of quantum mechanics (QM) and whether it must be considered "weird." Participants explore different interpretations and derivations of QM, questioning the assumptions underlying these views and their implications for understanding the theory.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants argue that presenting quantum mechanics as weird is detrimental to understanding, suggesting that it can be explained more intuitively.
  • One participant references a paper claiming to derive QM from reasonable assumptions but is challenged on the validity of its assumptions, particularly regarding measurement devices and the nature of quantum states.
  • Another participant emphasizes the distinction between interpretation and derivation, arguing that interpretations like the ensemble interpretation are incomplete but not necessarily incorrect.
  • Concerns are raised about the implications of assuming observations in the derivation of QM, particularly in relation to historical processes like the formation of the Sun.
  • Participants discuss the validity of using the ensemble interpretation as a basis for derivation, with some asserting that it leads to logical inconsistencies.
  • There is a contention regarding whether a conceptualization can be considered a valid derivation if it relies on invalid assumptions.
  • A later reply introduces a more philosophical perspective on the nature of reality in quantum mechanics, suggesting that the more one contemplates QM, the weirder it appears.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation and derivation of quantum mechanics, with no consensus reached on whether QM must be considered weird or the validity of specific derivations based on the ensemble interpretation.

Contextual Notes

Participants highlight limitations in the assumptions made in various derivations, particularly regarding the role of measurement devices and the implications for understanding quantum states in the absence of observations.

  • #541
stevendaryl said:
Bell discussed a toy model for EPR correlations in which the "hidden variable" was a hemisphere, and Alice measured spin-up if she chose an axis in that hemisphere, and spin-down if she chose an axis not in that hemisphere. That model does not replicate the predictions of QM.
Agreed, I have come across this too. I believe that the toy model assumes a direction that is predetermined in all three directions. My toy model assumes that it is only predetermined in one.
 
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  • #542
rubi said:
Well, it misses the point of Bell's theorem, because it is supposed to miss the point of Bell's theorem. Bell wants to exclude deterministic hidden variables and the violation of the inequality shows that he was successful. It's not about finding a loophole in Bell's argument, I happily reject deterministic hidden variables. The point of the contextual model is to offer an alternative explanation to deterministic hidden variables, while still maintaining locality. The question is: Is there an apriori reason to exclude contextual probabilistic models like the one I described in post #530? If not, then either we can show that these models are incompatible with QM as well (which I doubt), or we are unable to claim that QM violates locality.

As far as I'm concerned, the way Bell defined locality excludes the sort of contextual hidden variables you're describing: the point is to be able to explain correlations in terms of some common origin or past interaction, described by variables ##\lambda##, and variables that don't have a value independently of the choice of measurement aren't useful for this purpose. But if you define locality differently than Bell did then of course the result can be different.

If you want to argue that we should be OK with a type of contextual local model that is more general than Bell then you need to consider why one might want an alternative model to quantum physics in the first place. If you look at Bell's reasons, he criticised quantum physics for being too vague and badly defined, specifically describing what we would nowadays call the measurement problem. From this perspective I think contextuality doesn't even qualify as a well-defined physical concept since, for me, if you call a model "contextual" you're basically admitting it will have the same sort of measurement problem as quantum physics does.
 
  • #543
stevendaryl said:
No, I wasn't arguing for that. What I assumed, as I said in an earlier post, was:
  1. There is a single random variable, \lambda, associated with the twin pair. This is chosen according to some probability distribution, P(\lambda).
  2. When a particle reaches Alice, she has already picked a measurement setting \vec{a}, and her device is already in some state \alpha. Then she will get result +1 according to some probability P_A(\vec{a}, \alpha, \lambda) that depends on \vec{a}, \alpha and \lambda.
  3. Similarly, when the other particle reaches Bob, he will get result +1 according to some probability P_B(\vec{b}, \beta, \lambda) that depends on \vec{b}, \beta and \lambda, where \vec{b} is his detector's setting, and \beta is other facts about his detector.
There is no assumption of determinism here. But there is no way to reproduce the perfect anti-correlations predicted by QM unless Alice's and Bob's results are deterministic functions of \lambda, \vec{a} and \vec{b}, or unless there are nonlocal interactions (so that P_A may depend on facts about Bob, or P_B may depend on facts about Alice).

In this paper by C.S. Unnikrishnan http://arxiv.org/pdf/quant-ph/0407041.pdf
" If both analyzers were set to the same direction a=b the (anti) correlation is perfect according
to the conservation of angular momentum "
And later he shows that P (a,b)c = - ab = P(a,b)QM = -cos (θ)
 
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  • #544
Jilang said:
Agreed, I have come across this too. I believe that the toy model assumes a direction that is predetermined in all three directions. My toy model assumes that it is only predetermined in one.

Well, I don't see how that could possibly work. It would be nice to see you work out the mathematics to show what such a model predicts for correlations.
 
  • #545
Closed pending moderation

Edit: the thread has outlived its usefulness and will remain closed
 
Last edited:

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