What grade of decoherence to be a classical aparatus

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    Classical Decoherence
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Discussion Overview

The discussion revolves around the concept of decoherence in quantum mechanics and its implications for defining classical measurement apparatuses. Participants explore the conditions under which a quantum system's wavefunction can be considered to collapse and how this relates to the density matrix's non-diagonal elements. The conversation touches on both qualitative and quantitative aspects of decoherence and classicality.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants suggest that a classical apparatus must "quasieliminate" the non-diagonal elements of the density matrix, but they express uncertainty about the specific conditions required for this process.
  • Others argue that the analysis of decoherence should focus on the strength and duration of the interaction with the environment rather than the size of the measuring devices.
  • A participant notes that while the density matrix approaches a diagonal form, it never becomes completely diagonal, indicating that decoherence is a gradual process.
  • There is a discussion about the ambiguity of the term "quasiclassical wavefunction," with some participants stating that it is difficult to definitively categorize a wavefunction as quasiclassical.
  • One participant proposes that if an apparatus is perceived as classical, then systems that are more classical than it may also behave classically, suggesting a provisional solution to the measurement problem.
  • Another viewpoint emphasizes that classical measurement devices typically have many degrees of freedom, leading to a rapid decay of off-diagonal terms in the density matrix, which contributes to their classification as classical.
  • Participants mention external resources and ongoing discussions related to decoherence times and their implications.

Areas of Agreement / Disagreement

Participants express a range of views regarding the definitions and implications of decoherence and classicality, indicating that there is no consensus on how to categorize wavefunctions or measurement devices as classical.

Contextual Notes

Participants highlight the limitations in defining "quasiclassical wavefunction" and the challenges in establishing a standard way to categorize systems as classical. The discussion reflects the complexity and nuance involved in understanding decoherence.

StarsRuler
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Books of quantum mechanics are very ambigous in this aspect. A classical apparatus that collapse wavefunction of a quantum system must "quasieliminate" the non-diagonal elements of density matrix, or have a quasiclassical wavefunction of the form
[itex]ae^{iS\hbar^{-1}}[/itex] where a is a real slowly changing in space and time and S is the classical action in the trayectory between 2 points of the wavefunction. But ¿ how much slow this change of a, and rapid oscillating S ?. There is qualitative but no quantitative answers in both forms of watch a classical system, in particular a measurement apparatus
 
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I think the analysis is done in terms of the strength and time of the interaction with the environment, not in terms of the size of the measuring decives.
 
books on QM are ambiguous exactly because decoherence is a concept based on a certain limit. In other words, as the classical apparatus causes the density matrix to tend to a diagonal matrix, the system decoheres more and more. generally, the density matrix will never become completely diagonal, but as it becomes closer to being diagonal, so too the system becomes more decoherent.

edit: and generally, there is no standard way to categorise the system to say if it is classical. And the definition 'quasiclassical wavefunction' also suffers from the same problem of being arbitrarily defined. In truth, we can only say that one wavefunction is more 'quasiclassical' than another. We cannot definitively say that a wavefunction is quasiclassical. This is pretty much the main idea of the measurement problem.

second edit: I guess you can say that a wavefunction tends to a quasiclassical wavefunction under a certain limit.
 
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We cannot definitively say that a wavefunction is quasiclassical. This is pretty much the main idea of the measurement problem.

And what is done in praxis? If a certain apparatus is perceived like a classical system, then all the systems more classical than it we can be sure that his comportment will be classical too, I suppose. Is this the provisional solution to the problem??
 
hmm. That makes sense to me. I think in most cases, classical measurement devices have such a large number of degrees of freedom that the off-diagonal terms of the density matrix decay very quickly, so that people just say "it is a classical apparatus" without putting much thought into it. another thing that could be considered is how easily quantum information leaks from the apparatus to its environment.

There is another thread going on, where someone called audioloop has given some nice links to some research into decoherence times, e.t.c. on pages 7 and 8 of this thread: https://www.physicsforums.com/showthread.php?t=682271&page=7 you might find these interesting.
 

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