Wheeler's delayed choice doesn't change the past

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Discussion Overview

The discussion revolves around Wheeler's delayed choice experiment and its implications for the nature of reality, causality, and the interpretation of quantum mechanics, particularly in relation to Feynman's path integral formulation. Participants explore the philosophical and technical aspects of how observations affect the understanding of past events in quantum mechanics.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • One participant argues that Feynman's path integral approach captures aspects of reality better than other interpretations, emphasizing that multiple paths do not correspond to actual single stories in time.
  • Another participant asserts that the delayed choice does not change the past but allows for postselection of observed properties, referencing a discussion from their habilitation defense.
  • A third participant references their own work to support the claim that delayed choice experiments do not alter past events.
  • Concerns are raised about Hawking's assertion that observations affect the past, with one participant expressing skepticism about this interpretation.
  • Another participant quotes Wheeler, suggesting that the concept of "reality" is contingent upon measurement and that the past exists only as recorded in the present.
  • Multiple participants express astonishment at Hawking's claims, questioning the validity of the assertion that observations can influence the past.

Areas of Agreement / Disagreement

Participants generally agree that delayed choice experiments do not change the past, but there is disagreement regarding the implications of observations on the nature of reality and past events. The discussion remains unresolved with competing views on the interpretation of quantum mechanics and the role of observation.

Contextual Notes

Participants highlight limitations in understanding due to the complexity of quantum mechanics and differing interpretations of the delayed choice experiment. Some references to external works and discussions may not be fully accessible to all participants.

  • #151
I know this, but how can a physicist write a pamphlet against measurements? Even a theoretical physicist gets unemployed if there are no measurements done anymore (except he can switch to pure mathematics or, horribile dictu, philosophy ;-)).
 
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  • #152
vanhees71 said:
I know this, but how can a physicist write a pamphlet against measurements?
Bell, of course, is not against doing measurements, or against using the results of measurement to formulate the theory. He is against measurement as a part of formulation of the theory. In classical mechanics, measurement is not a part of the formulation of the theory. In standard quantum mechanics, it is.
 
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  • #153
In classical mechanics already writing down a position vector in terms of its Cartesian components implicitly assumes measurements.
 
  • #154
vanhees71 said:
In classical mechanics already writing down a position vector in terms of its Cartesian components implicitly assumes measurements.
I don't think so, just as I don't think that decomposing a quantum state in a specified basis for the Hilbert space implicitly assumes measurement.
 
  • #155
vanhees71 said:
Well, of course, to measure the position of a particle you need a different device than to meausure its momentum. This is not specific to QT but also the case within classical physics. Indeed there's no problem with this, and it's in no way mystical at all.
The difference is that in classical mechanics you an in principle have several measurement devices at once, measuring all things at once without distorting the system. Ie. you can have a "collection of observers" asking all kinds of questions at once, and then simlpy joing the answers.

This is not possible in quantum mehanics, and its Bohrs point with complementarity.

In this case the measurent is "trivial" or marginalized to a practical matters in classical matter. In quantum mechanics, the choice of measurements distorts the system, in a way that that dependes on what you choose to measure. This is the "subjectivity".

But there is no point in disagreeing on the word. I think we roughly agree at the basic level. I just wanted to express that even though i may not share Demystifiers view, i still follow the objections and point of subjectivity (give or take the choice of words).
vanhees71 said:
I've also never understood Bohr's "classical measurement device". According to QT everything is quantum, including macroscopic systems making up measurement devices. The classical behavior of the relevant macroscopic observables (which are coarse-grained by averaging many microscopic degrees of freedom over microscopically large, macroscopically small space-time regions) is emergent.
You can not in Borhs view properly speak of what is quantum without a classical reference. Surely, you can view the apparatous + system as another "new quantum system" BUT, then you need ANOTHER classical backdrop. To think you can repeat this until you end up with a complete wavefunction of the universe is IMO a fallacy that makes no sense. I think this is Bohrs point. But if we get into the details here, atl east i will raise questions that i think is beyond the scope of the original Einstein Bohr dispute. Bohrs point is I think the most acccurate one if you consider quantum theory as it stands. Even field theory needs a backdrop. The detectors must be attached in a classical world.

To generalized things beyond that, then we are at BTSM discussions.

There is IMO also a connection between when the Newtonian schema works (as per Smolin) AND Bohrs requirement for aclassical backdrop. Without the classical backdrop, which also severs the purposes of information sink, there is no rigid reference for the Newtonian schema - and we need a new understanding of physical law.

/Fredrik
 
  • #156
We don't need a revolution of physics. It already happened in 1926 with the discovery of quantum theory (in 3 equivalent forms) and Born's probabilistic interpretation of the quantum state. There's no need for any other revolution since QT works very well in describing all known phenomena.
 
  • #158
Thread permanently closed. Original question answered - now just a discussion of different views of physics.
 
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