Which interpretation best explains the classical limit?

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Discussion Overview

The discussion centers on the classical limit of quantum mechanics, exploring whether various interpretations of quantum theory, such as Bohmian mechanics and the many worlds interpretation (MWI), adequately explain the transition from quantum behavior to classical behavior, particularly in the context of macroscopic objects like a tennis ball. The conversation touches on theoretical implications, experimental observations, and the measurement problem.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants suggest that the classical limit poses a 'real problem' for quantum physics, particularly in reconciling quantum mechanics with classical observations, such as the behavior of a tennis ball.
  • One participant mentions Ehrenfest's theorem as a means to recover classical laws from quantum mechanics, noting its effectiveness for macroscopic particles but also its limitations when wave functions spread.
  • Another participant emphasizes that Ehrenfest's theorem can predict the motion of large mass particles like tennis balls, asserting that it aligns with Newton's laws under certain conditions.
  • There is a discussion on the differences between interpretations, with some arguing that Bohmian mechanics provides a more straightforward derivation of the classical limit compared to MWI, which raises questions about how quantum states translate into classical perceptions.
  • One participant claims that all interpretations yield the correct classical limit, but questions whether critics of Bohmian mechanics would agree on its directness in deriving this limit.

Areas of Agreement / Disagreement

Participants express differing views on the adequacy of various interpretations in explaining the classical limit. While some agree on the utility of Ehrenfest's theorem, others challenge its applicability and the implications of wave function behavior. The discussion remains unresolved regarding the best interpretation for explaining the classical limit.

Contextual Notes

Limitations include the dependence on the localization of wave functions and the specific conditions under which Ehrenfest's theorem applies. There are also unresolved questions about the implications of wave packet spreading and the nature of quantum state perceptions in different interpretations.

Starbug
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Trying decide, apropos that famous Feynman quote, whether there is a 'real problem' with quantum physics. My own rather inexpert view is that if there is, the it's something to do with the classical limit. (The measurement problem being an interesting special case of this.)

In particular because this is a substantive and indeed experimental problem. Although you wouldn't normally think that when I pick up a tennis ball and throw it across the room that this constitutes experimental refutation of quantum mechanics, I think that unless the phenomena has been adequately explained within the framework of quantum physics then that is just what it is.

There might be such an explanation of course I just don't know what it is. On the face of it though it must be quite challenging reconciling such different descriptions of the world. Although on the other hand I suppose this is not so strange, we're familiar with the idea that the system can be explained by different laws depending on what the observables are, e.g thermodynamics is the appropriate theory if the observable is temperature and pressure and so on. This is sometimes called "emergence" although that may refer to something more specific. Anyway in the instance of me throwing a tennis ball I suppose the relevant observable is something like the center of mass motion and we some explanation for why such macroscopic observables like this obey classical physics.

I'm also interested especially in comparing how Bohmian mechanics and the many worlds interpretation deal with this question. It's been argued that it's an important virtue of Bohm's theory that the classical limit question is straight-forward, since the classical position variables are in from the start and go all the way down so to speak. Whereas in the MWI, an otherwise quite similar interpretation, the quantum state comes all the way up. I have difficulty understanding how the quantum state of the whole universe gets sliced up in our perceptions into the classical world we observe.

Any thoughts?
 
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Ehrenfest's theorem gives you back Newton's laws and the usual classical equations for momentum and energy and so on. These predict the motion of a tennis ball pretty well.
 
ironhill said:
Ehrenfest's theorem gives you back Newton's laws and the usual classical equations for momentum and energy and so on. These predict the motion of a tennis ball pretty well.


The Ehrenfest's theorem works only when the support of the wave function is localized on a macroscopic level. Unfortunately the wave function has a stubbon tendency to spread. Thus for example, by applying the Ehrenfest's theorem to a particle which crosses a beam splitter we obtain a very strange trajectory, that mediates the transmitted and the reflected trajectories. Not to mention what happen when also the detectors behind the transmitted and reflected beams are taken into account...
 
The question of how a large mass particle, like an ideal tennis ball, behaves is goverened adequetly by Ehrenfest's theorem. Spreading of a wavepacket is essentially nil (for a Gaussian wavepacket I think there's a factor (h/m)^2 can't remember offhand, it's in Merzbacher). If you want to talk about light then naturally it won't work because you are dealing with an inherently quantum phenomenon.

My understanding of what the OP was implying, only his second paragraph, was that quantum mechanics doesn't predict the trajectories of large particles, like tennis balls. However in this case Ehrenfest works, you get Newtons equations and the usual laws of projectile motion.
 
All interpretations give the correct classical limit.
Nevertheless, even those who do not like the Bohmian interpretation cannot disagree that in this interpretation the derivation of the classical limit is the most direct.
(Or can they?)
 

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