Find a calculation of Schrödinger's cat experiment?

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Discussion Overview

The discussion revolves around the Schrödinger's cat thought experiment, focusing on the possibility of calculating its quantum state and the implications of quantum mechanics on the understanding of superposition and measurement. Participants explore theoretical aspects, interpretations of quantum mechanics, and the philosophical implications of the experiment.

Discussion Character

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

Main Points Raised

  • Some participants inquire about calculations related to Schrödinger's cat, suggesting that a detailed calculation is impractical due to the complexity of the particles involved.
  • It is noted that Schrödinger's original intent was to highlight issues with the understanding of quantum mechanics rather than to propose that a superposition of dead and alive states occurs.
  • Participants mention the concept of quantum decoherence as a significant development in understanding the measurement problem in quantum mechanics.
  • One participant references a paper by A.J. Leggett discussing the limits of quantum mechanics and the implications of different interpretations of quantum theory.
  • There is a discussion about the nature of the quantum state of the cat, with some suggesting that it represents "quantum ignorance" rather than a definitive physical state.
  • Participants express caution regarding interpretations of superposition, debating whether it can be understood as a probability of the cat being alive or dead.
  • Some participants refer to recent experiments that may demonstrate Schrödinger cat states, indicating ongoing research in this area.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the interpretation of the quantum state of the cat or the implications of superposition. Multiple competing views remain regarding the nature of quantum mechanics and its relationship to reality.

Contextual Notes

Limitations include the complexity of calculating the state of the cat and the unresolved nature of interpretations of quantum mechanics, particularly concerning the transition from quantum to classical states.

  • #31
True, but you cannot treat the Geiger counter by solving the Schrödinger wave equation exactly for its ##10^{30}## (or so) constituents, and it is indeed completely sufficient to treat the relevant physics of the Geiger counter in terms of classical physics. It's misleading to write ##|\text{decay measured} \rangle## since the observation that a decay has been registered is not a microscopic but a macrscopic observable. Here lies the key for the understanding that there is no measurement problem, and this was emphasized already by Bohr in the early days of QT.

To understand theoretically, why the classical description of the macroscopic observables of macroscopic systems is a valid approximation of QT, you need quantum statistics or "many-body theory". That's all I'm saying.
 
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  • #32
vanhees71 said:
True, but you cannot treat the Geiger counter by solving the Schrödinger wave equation exactly for its ##10^{30}## (or so) constituents, and it is indeed completely sufficient to treat the relevant physics of the Geiger counter in terms of classical physics. It's misleading to write ##|\text{decay measured} \rangle## since the observation that a decay has been registered is not a microscopic but a macrscopic observable. Here lies the key for the understanding that there is no measurement problem, and this was emphasized already by Bohr in the early days of QT.

To understand theoretically, why the classical description of the macroscopic observables of macroscopic systems is a valid approximation of QT, you need quantum statistics or "many-body theory". That's all I'm saying.

There lies no key for the understanding that there is no measurement problem. You are simply making an artificially cut between – whatever you call it – “microscopic” and “macroscopic” observables - quietly and secretly assuming that somewhere a "collapse" or "reduction" occurs.

To say it in terms by Landau and Lifshitz: “Thus quantum mechanics occupies a very unusual place among physical theories: it contains classical mechanics as a limiting case, yet at the same time it requires this limiting case for its own formulation.”
 
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  • #33
Well, LL is right with that, but I don't consider this as a problem, because QT contains classical mechanics as a limiting case. So there is no contradiction between classical and quantum theory, where the classical approximation is valid. Of course, there is no fundamental "cut". QT is more comprehensive than classical theory, and the better our preparation procedures become, thanks to technological progress, the larger systems can be shown to behave according to QT, e.g., there have been double-slit interference demonstrations by Zeilinger's group for fullerene molecules and as well the demonstration that already a pretty small temperature is enough to destroy the quantum interference due to decoherence because of the emission of just a few thermal photons.
 
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  • #34
vanhees71 said:
True, but you cannot treat the Geiger counter by solving the Schrödinger wave equation exactly for its ##10^{30}## (or so) constituents, and it is indeed completely sufficient to treat the relevant physics of the Geiger counter in terms of classical physics. It's misleading to write ##|\text{decay measured} \rangle## since the observation that a decay has been registered is not a microscopic but a macrscopic observable. Here lies the key for the understanding that there is no measurement problem, and this was emphasized already by Bohr in the early days of QT.
Okay, I now get the idea of taking it as an paradox free macroscopic thing. Before talking with you about the classical limit or black holes I surely need to learn more advanced QT first ...

Thanks everyone for taking so much time to explain it to me in detail!
 
  • #35
vanhees71 said:
So there is no contradiction between classical and quantum theory, where the classical approximation is valid.

In fact a careful analysis shows the real basis of classical mechanics is QM - but that is a whole new story and another thread if anyone wants to pursue it either here or on the classical physics sub-forum.

Thank
Bill
 

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