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Measurement of a quantum observable (in an appropriate, old-fashioned sense) necessarily involves coupling to a system with a macroscopically large number of degrees of freedom. Entanglement with this "apparatus" takes care of the decoherence. It is often said (I can provide references upon request) that the remaining problem is the one of "selection", and this is the point where one invariably invokes something philosophically radical, like many-worlds interpretation.

In the above (pretty standard) context, I am trying to make sense of the following observation. Looking at the measuring system from a statistical mechanics point of view, it seems that triggering a particular macroscopic outcome requires spontaneous symmetry breaking via a (thermodynamically) irreversible transition of the "apparatus" from a metastable to a higher entropy final state. My attitude is that "statistical mechanics point of view" is not far from "decoherent large quantum system".

So, the question is:

Is it fair to say that statistical irreversibility ("the second law") and quantum measurement irreversibility (the "wave-function collapse") are necessarily linked? Can this link be made more concrete (e.g., traced in details in a particular model)? Can you give references to approaches to the measurement problem that explore this connection?

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This question has an open bounty worth +50 reputation from Numrok ending in 2 days.

One or more of the answers is exemplary and worthy of an additional bounty.

Quantum statistical irreversibility ("the second law") and quantum measurement irreversibility are almost the same thing. Indeed,the latter is the special case of the former where one assumes a more specific situation in which you consider the statistical mechanics of a small system coupled to a large one. Equilibrium and nonequilibrium statistical mechanics, where one studies a single large system only, are other special case of general quantum statistical irreversibility.

The techniques used (essentially the projection operator formalism and its variants) are essentially the same in every case, but each kind of system has its own specialties.

See, e.g., the arXiv papers cond-mat/0102428 and cond-mat/0203460 for some exactly solvable problems that shed light on your problem.

For more details in the general case see the discussions at http://www.physicsoverflow.org/35537 and https://www.physicsforums.com/threads/collapse-from-unitarity.860627/

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@Numrok: see also the new references at the end! – Arnold Neumaier Jun 23 at 16:49
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@Slaviks: Could you please indicate why you unaccepted my answer? If possible with references to papers that made you discontent with my answer! – Arnold Neumaier Jun 23 at 16:50
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@Numrok: I like the statistical physics book by Linda Reichl. (Different editions vary a great deal; maybe look at several of them!) – Arnold Neumaier Jun 26 at 10:54
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For the classical side, see also Oettinger, Beyond equilibrium thermodynamics. – Arnold Neumaier Jun 26 at 10:55
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For the quantum side, see also Calzetta and Hu, Nonequilibrium quantum field theory. – Arnold Neumaier Jun 26 at 11:00

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