From: *smitra* <[email protected] <mailto:[email protected]>>

I guess I need to explain my point a bit better, so I'm starting from the beginning and will then address your points. We know that QM is non-deterministic as far as measurements results are concerned, one can ask if there exist hidden variables that would fix that problem in a local way using local hidden variables. Bell's theorem combined with the QM prediction (or you could invoke Aspect's experimental results confirming the predictions of QM) rules out any such fix.

So, all that Bell's theorem implies is that QM is incompatible with local hidden variables. This then means that measurements generate new information. If you measure the z-component of a spin polarized in the x-direction then after the measurement, one bit of information appears locally at your place (Bell's theorem rules out that this bit of information was not somehow already present locally at your place).

It is at this point where MWI differs from single World collapse theories. In the MWI, the state evolves into a superposition where both outcomes are realized, that superposition doesn't contain more information than the initial state. But each member of the superposition where there are definite measurement outcomes contain one bit of information more than the entire superposition. So, in the MWI, information appears due to copies of observers, analogous to what happens in Bruno's thought experiment, instead of really new information popping into existence physically as would be the case in a collapse interpretation.

New information 'pops into existence' for every observer in MWI, exactly as in a collapse model. So I don't see much significance in your point.

In case of entangled spins being measured at two space-like separated places with identical polarizer setting, only one bit of information will appear, but this will happen at two space-like separated places. In collapse interpretations this is a benign but strange non-local effect. Bertlmann's sock-type explanations don't work here because that would require the existence of information about the measurement results prior to the measurements already being present locally. Bells' theorem rules that out.

Actually, Bell's theorem does not rule out a local hidden variable account of the case for aligned polarizers. But this is not relevant for the general case of non-aligned polarizers. In that case Alice's measurement does not make one bit of information appear at Bob's location -- he can still get either up or down, and there is no way to tell which. What does change are the probabilities for these results. And those probabilities depend on the relative orientation of the polarizers, and that can only be known non-locally.

In the MWI things are different, because there is no new information that appears in the global final state. What happens is that the initial state evolves into a superposition that can be split into two components where the observers find their measurement results. These results are then correlated as a result of the evolution of the wavefunction.

As I keep saying. The wave function for the non-separable state is itself non-local. You cannot avoid non-locality by appealing to the evolution of the wave function.

You can then say that the wavefunction has non-local properties, therefore there is no difference between the MWI and collapse interpretations in this respect. However, in collapse interpretation the collapse is just an ad-hoc postulate without further explanation, while in the MWI it happens as a result of local dynamics, the non-local wavefunction involved here itself evolved allowing one to trace back the source of the non-locality right to the point where the entangled spins were created.

How does one do this trace-back? The reason that the EPR correlations cannot be explained locally is that the relative angle of the separated measurements cannot be accommodated in local hidden variables. Maudlin spends quite a lot of time exploring this in his book 'Quantum Non-Locality and Relativity'. Unless you have some means of determining the relative orientation of the polarizers in MWI that is not present in the single-world model, then you have not explained the correlations locally.

While one can then still argue that MWI does have non-local aspects to it because the branches do not split in a local way, for me what matters is that all such issues are explained by local dynamics,

Everett thought he had abolished all forms on non-locality when he discarded the collapse postulate. Schrödinger's concern about the non-locality of his wave theory was about precisely this -- pass a particle through a hole; the wave front expands spherically. But when it meets a screen, only one point is seen -- the rest of the wave appears to have mysteriously collapsed. Everett explains this by saying that things split into an (infinite) number of worlds, in each of which the spot on the screen appears in a different place. Overall there is no collapse -- it is just that for any particular observer it appears as though there has been because he sees only one of the infinity of spots.

This works fine for this sort of collapse. But it does not work for entangled particles -- the collapse in that case is independent of the separation, and depends on non-local details at both ends of the entanglement.

while in collapse interpretations you have more problems precisely due to the unexplained collapse. In collapse interpretations, new information appears right at the moment of collapse and does so non-locally in case of entangled spins. In the MWI, the branching is only an effective picture, the exact picture does not contain any branching. No new information appears in the global state. The self-localization of observers within this global state has non-local aspects to it, but there is an explanation for that that invokes only local dynamics.

But you still have not given a local account of how this happens. Spell out for me the local dynamics that lets the state that Bob measures reflect the relative angle between his and Alice's polarizers. It is all very well to appeal to the dynamics of the wave function. But those dynamics are non-local. You really do have to to better than this. Try writing out some equations rather that blanketing everything with imprecise words.

Bruce

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