Mathematical formulation of local non-realism

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Discussion Overview

The discussion revolves around the mathematical formulation of local non-realism in quantum mechanics, specifically focusing on the interpretation of probability distributions related to measurements of spatially separated particles. Participants explore the implications of local realism and non-realism, examining how these concepts can be expressed mathematically and what assumptions underlie these interpretations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents Bell's formulation of local realism and proposes a modified probability distribution for a theory that is realistic but not necessarily local.
  • Another participant argues that in a local non-realistic interpretation, the probability distribution ##P(a,b)## cannot exist if measurements are spatially separated, as there is no single observer to measure it.
  • There is a discussion on whether observers need to assume that the other remains in a superposition until results are compared, with some suggesting that non-realistic interpretations do not allow assumptions about unobserved phenomena.
  • One participant questions if a hardcore non-realist would need to consider themselves the only observer capable of making measurements, leading to a discussion on the implications of solipsism in this context.
  • Participants discuss the necessity for observer ##A## to compute correlations ##P(a,b)## based on local measurements, raising questions about the nature of unitary evolution and projective measurements in non-realistic interpretations.

Areas of Agreement / Disagreement

Participants express differing views on the implications of local non-realism and the nature of probability distributions in quantum mechanics. There is no consensus on how local realism and non-realism can be distinctly separated or how they should be mathematically formulated.

Contextual Notes

The discussion includes assumptions about the nature of measurements, the role of observers, and the interpretation of quantum mechanics, which remain unresolved. The implications of solipsism and the relationship between local and non-local interpretations are also explored but not definitively concluded.

greypilgrim
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Hi.

Bell formulated local realism as follows: The probability of a coincidence between separated measurements of particles with correlated (e.g. identical or opposite) orientation properties can be written as
$$P(a,b)=\int{d\lambda\cdot \rho(\lambda)\cdot p_A(a,\lambda)\cdot p_B(b,\lambda)}\enspace .$$

To get a better understanding of the terms "local" and "realistic", I'm trying to adapt this formula. So I'd say a theory that realistic, but not necessarily local, would satisfy
$$P(a,b)=\int{d\lambda\cdot \rho(\lambda)\cdot p_{AB}(a,b,\lambda)}\enspace ,$$
i.e. ##p_{AB}(a,b,\lambda)## is not necessarily a product distribution. As far as I can see quantum expectation values satisfy this probability distribution.

How would this formula look like for a nonrealistic (or not necessarily realistic), but local theory? Or is local realism not something that can be split up into locality and realism?
 
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If ##a## and ##b## are spatially separated, then, according to the local non-realistic interpretation, there is no such thing as ##P(a,b)##. Namely, there is no single observer who can measure ##P(a,b)##, and things which nobody measures don't exist according to non-realistic interpretations.

If ##a## and ##b## are not spatially separated and a single observer measures both ##a## and ##b##, then, according to the same interpretation,
$$P(a,b)=p_{AB}(a,b)$$
which is almost a tautology.
 
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Demystifier said:
If aa and bb are spatially separated, then, according to the local non-realistic interpretation, there is no such thing as P(a,b)P(a,b). Namely, there is no single observer who can measure P(a,b)P(a,b), and things which nobody measures don't exist according to non-realistic interpretations.
So in this interpretation it's not allowed that both observers make individual, spatially separated measurements and then construct ##P(a,b)## by comparing their results locally at a later time?

Do both observers need to assume the other one stays in a superposition until they compare their results over a classical channel?
 
greypilgrim said:
So in this interpretation it's not allowed that both observers make individual, spatially separated measurements and then construct ##P(a,b)## by comparing their results locally at a later time?
It's allowed, but then the observables that are really compared are no longer spatially separated. According to non-realistic interpretations, there is no correlation until one observes the correlation.

greypilgrim said:
Do both observers need to assume the other one stays in a superposition until they compare their results over a classical channel?
In non-realistic interpretations (I am not a proponent of such interpretations, I just explain what such interpretations are), you don't assume anything about things which you don't observe.
 
Demystifier said:
In non-realistic interpretations (I am not a proponent of such interpretations, I just explain what such interpretations are), you don't assume anything about things which you don't observe.
But in order to agree with experimentally verifiable QM predictions, observer ##A## needs a way to compute the correlations ##P(a,b)## that ##A## and ##B## will find when they later compare their measurements locally. So will he describe everything on ##B##'s side as a unitary time evolution (i.e. with local Hamiltonians) and only use projective measurements when they meet (or talk over a classical channel)?

If I was a hardcore non-realist, would I need to assume I'm the only one in the whole universe capable of making QM measurements and everything else evolutes unitarily?
 
greypilgrim said:
But in order to agree with experimentally verifiable QM predictions, observer ##A## needs a way to compute the correlations ##P(a,b)## that ##A## and ##B## will find when they later compare their measurements locally. So will he describe everything on ##B##'s side as a unitary time evolution (i.e. with local Hamiltonians) and only use projective measurements when they meet (or talk over a classical channel)?
Yes, exactly.

greypilgrim said:
If I was a hardcore non-realist, would I need to assume I'm the only one in the whole universe capable of making QM measurements and everything else evolutes unitarily?
That would be a kind of solipsism, and yes, I also think that hardcore non-realism leads to solipsism. See also
http://lanl.arxiv.org/abs/1112.2034
 

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