vanesch
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Ken G said:I think the lecturer must have meant "cannot be entangled with another particle if we are to use this analysis," rather than "it is impossible for further entanglements to exist." In principle, particles are vastly mutually entangled, including the fact that many are indistinguishable in the first place (like all electrons, etc.). But physics is not about what is, it is about how we can treat what is and get the right answers, to within some desired precision. In practice, we can find situations where entanglements are vastly unimportant, or we can find situations where simple entanglements matter but more complicated ones don't. Physics is very much about building up to the complex from the simple, and that it works at all says something about what a tiny fraction of the information the universe encodes is actually "active" in determining the outcomes of our experiments.
Indeed. I think we said this already before in this thread: massive entanglement gives in most cases exactly the same observable result as no entanglement. This is why there are families of interpretations of quantum mechanics which go for the "no entanglement" view (all projection-based interpretations), and those that go for the "massive entanglement" view (all MWI-like interpretations). The link between both is decoherence.
When you look at quantum dynamics, when two subsystems interact, most of the time this results in an entangled state between both, even if initially, we had "pure product states", that is to say, each system had its own independent quantum state, and the overall state was just the juxtaposition of these two sub-system states. As it is very difficult to deny a system to interact with its environment (scatter a thermal photon, hit a molecule of air, interact with a phonon in a solid - a vibration - ...), usually a system quickly gets entangled with its environment (if you follow quantum dynamics). Turns out that you can ONLY distinguish entangled states from statistical mixtures of pure product states if you do a correlation measurement on ALL entangled components in a ROTATED measurement basis. If you omit one, the remaining correlation will show up as identical to that of a statistical mixture.
So if your system hit a remaining air molecule, scattered a thermal photon, and created a phonon in a crystal of the metal of your vacuum tube, then in order to see this entanglement, you'd have to measure simultaneously your system, that air molecule, that photon, and that phonon, in an incompatible basis with the original one. FAPP, that's impossible. So FAPP, your system is now in a statistical mixture of pure product states, EVEN if it contained entangled components (that is to say, your system was 2 or more subsystems on purpose).
So you can now say that the "measurement" has "projected out" the states of the system (and you have a statistical mixture of measurement outcomes) - that's Copenhagen and Co ; or you can say that your system got hopelessly entangled with its environment (including you): that's MWI and Co. The last approach has the advantage that it follows from quantum dynamics directly and is why personally, I like it. But the results are the same: no weird correlations are seen from the moment there is interaction with the environment.
This is why entanglement experiments are hard and never done with cats.