Popper/Lande interpretation of QM

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    Interpretation Qm
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Discussion Overview

The discussion centers on Karl Popper's "propensity field interpretation" of quantum mechanics, as presented in his 1982 work. Participants explore the implications of Popper's critique of the Copenhagen interpretation, the nature of quantum mechanics, and the relationship between particles and their statistical descriptions. The conversation touches on theoretical interpretations, critiques of established views, and the philosophical underpinnings of quantum mechanics.

Discussion Character

  • Debate/contested
  • Exploratory
  • Technical explanation

Main Points Raised

  • Some participants highlight Popper's critique of the Copenhagen interpretation, emphasizing his argument for a realist, particle-based view of quantum mechanics.
  • Others note that Popper's interpretation suggests that the wave function is merely a mathematical tool rather than a physical property of particles.
  • Some argue that the concept of wave/particle duality is misleading and that propensity fields are properties of experimental arrangements rather than particles themselves.
  • A participant mentions that Popper's critique may not hold up against Bell's Theorem and entanglement experiments, suggesting a need to align with Bohmian interpretations for coherence.
  • Another participant draws parallels between Popper's theses and the statistical ensemble interpretation of quantum mechanics as discussed by Ballentine.

Areas of Agreement / Disagreement

Participants express differing views on the validity and implications of Popper's interpretation. There is no consensus on the critique of the Copenhagen interpretation or the acceptance of the propensity field model as a more common-sense approach to quantum mechanics.

Contextual Notes

Some participants reference the limitations of Popper's arguments in light of contemporary developments in quantum mechanics, such as entanglement and Bell's Theorem, which may challenge his conclusions.

  • #31
DrChinese said:

Thanks for the link. Interesting article. It looks consistent to me, and I appreciate the quote by a philosopher :). I find it especially interesting that this description of BI avoids the falsified causal implications of classical properties by simply denying the existence of any classical properties with causal implications.

"Just as psi is no classical field, the Bohmian particles are no classical particles. i.e., they are no bearers of properties other than position. ... Agreed, this is a radical departure from the classical particle concept."

Doesn't personally do it for me, but as far as I can tell it's perfectly viable and as provable as other self-consistent theories. I'll save the semantic arguments for a different forum (they aren't as interesting anyways).
 
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  • #32
DaleSpam said:
Not necessarily. You can easily have any two of FTL, relativity, and causality. An instantaneous action may be relativistic, in which case it would violate causality in some reference frames.

DaleSpam,

I'm glad you brought this up. It shows our differences in assumptions. I would argue that relativity and locality are synthetic propositions while causality is an analytic truth. That a cause must precede its effect is guaranteed by the definitions of the words cause and effect, putting it on the same level as 1+1=2.

A theory can still comply with the tautological truth of causality by redefining time - by redefining what it means for one event to precede another. Doing this, however, gives you a definition of time inconsistent with time in relativity.

So I have been assuming that, at least without throwing out relativity, causality must be true. Without this assumption I would agree with all of your previous statements.
 
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  • #33
kote said:
... I would argue that relativity and locality are synthetic propositions while causality is an analytic truth. That a cause must precede its effect is guaranteed by the definitions of the words cause and effect, putting it on the same level as 1+1=2.

A theory can still comply with the tautological truth of causality by redefining time - by redefining what it means for one event to precede another...

I would agree that assuming causality is tautological. And the evidence is fully consistent with the ideas that a) there are NO causes; or b) the future influences the past.
 
  • #34
kote said:
Special relativity is a statement of locality. Relativity is locality.
No it isn't. If it were, then we would not have two different words for the same thing.
 
  • #35
DrChinese said:
And the evidence is fully consistent with the ideas that a) there are NO causes; or b) the future influences the past.
I would say that both a) and b) are true. Let me explain.

What does it mean that A is cause of B? It means a logical relation
A -> B
i.e., A IMPLIES B.
But what if both
A -> B
and
B -> A
are true?
Should we say that then A is a cause of B and B is a cause A? I don't think so. It's better to say that the notion of cause and consequence do not have any fundamental meaning. (They have only meaning on an effective macroscopic level, due to the second "law" of thermodynamics.)
 
  • #36
Demystifier said:
I would say that both a) and b) are true. Let me explain.

What does it mean that A is cause of B? It means a logical relation
A -> B
i.e., A IMPLIES B.
But what if both
A -> B
and
B -> A
are true?
Should we say that then A is a cause of B and B is a cause A? I don't think so. It's better to say that the notion of cause and consequence do not have any fundamental meaning. (They have only meaning on an effective macroscopic level, due to the second "law" of thermodynamics.)

I think cause and effect is a convenient concept for helping us to decide how to act. It provides a sense of personal responsibility. I don't think it is a rigorous scientific truth.
 
  • #37
DrChinese said:
I think cause and effect is a convenient concept for helping us to decide how to act. It provides a sense of personal responsibility. I don't think it is a rigorous scientific truth.
So we basically agree on that issue. :smile:
 

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