PeterDonis said:
Btw, I should make it clear that this is not a criticism of you (
@DrChinese) for asking the question. If it's a criticism of anything, it's a criticism of the literature that has focused so much attention on terms like "locality" when much, if not most (maybe even
all) of that discussion boils down in the end to people using the same word with different meanings and talking past each other.
We've had this discussion before, true, and you seem to feel there is more ambiguity in the term "local" and "locality" than most authors.
a) If I can send signals faster than c (which is impossible as we know it), that violates locality.
b) If 2 entangled particles exert a mutual influence on each other when they occupy a region of space, that violates locality.
c) If a measurement on one of 2 entangled particles causes a remote change to its distant partner, that violates locality - even if the change itself has a random character which cannot be controlled sufficiently to send any useful information.
d) If I can teleport a quantum state from one quantum system to another sufficiently distant, that violates locality.
e) If I can remotely change a quantum state sufficiently distant, that violates locality.
On the other hand: if there is a local mechanism which can explain any of the criteria above, then that criterion should be struck. I don't think we need to worry about a) as there is no point of disagreement on this. The others may or may not be issues, depending on the MWI perspective. Obviously, there are experiments which demonstrate d) and e). Of course, it is not unusual for proponents of an interpretation to simply deny the validity of experiments which appear to go against their preference.
I think a reasonable experimental reference is:
High-fidelity entanglement swapping with fully independent sources
https://arxiv.org/abs/0809.3991
Rainer Kaltenbaek, Robert Prevedel, Markus Aspelmeyer, Anton Zeilinger
"Entanglement swapping allows to establish entanglement between independent particles that never interacted nor share any common past. ..."
I'd like someone to explain how this specifically works under MWI without invoking any kind of nonlocal action or global variables. And if the answer is to deny the published paper, well, that doesn't really explain anything in my book.
I'm perfectly good with starting out photons 1/2/3/4 having some kind of spreading wave function. I am also good with the idea that a polarization measurement of photon 1 (say) splits things into 2 versions (worlds, universes, histories, wavefunctions, wave states or whatever we want to call it). In one world, the Photon 1 polarization is now H> and in the other world it is V>. According to one source on MWI: "
The wavefunction obeys the empirically derived standard linear deterministic wave equations at all times. The observer plays no special role in the theory and, consequently, there is no collapse of the wavefunction."
Presumably, if MWI is local (or localized or whatever you might call it): during their short life span, photons 1 & 4 never come close to each other. They are not synchronized (entangled) with each other initially. The swapping operation on photons 2 & 3 can occur distant to both 1 and 4. So how do 1 & 4 become entangled when they are far from each other (and far from 2&3 as well) ? In other words, at what point should we expect to see worlds in which the 1 & 4 photons are showing entangled outcomes? And at what point did their "
deterministic wave equations" overlap or interact with each other in a manner that allows them to be synchronized?
Thanks,
-DrC
PS Keep in mind, I don't know how it really works in any interpretation, other than I believe there is a nonlocal component of some kind involved that explains one or more of the criteria I presented.