On 14/11/2017 10:01 am, Brent Meeker wrote:
On 11/13/2017 1:40 PM, Bruce Kellett wrote:
On 14/11/2017 2:07 am, Bruno Marchal wrote:
On 12 Nov 2017, at 23:05, Bruce Kellett wrote:

What really annoys me is the continued claim that many worlds eliminates the need for non-locality. It does not, and neither Bruno nor anyone else has ever produced a valid argument as to how many worlds might restore locality.

But nobody has proved that there is non locality in the MWI. EPR-BELL proves non-locality apparant in each branch, but the MWI avoids the needs of action at a distance to explains them. Once Alice and Bob are space-separated, their identity are independent. It makes no sense to talk of each of them like if they were related, (unless you correlate them with a third observer, etc) If they do measurement, some God could see that they are indeed no more related, but if they decide to come back to place where they can compared locally their spin, they will always get contact to the corresponding observer with the well correlated spin. The independent Alice and Bob will never meet because they can't belong to the same branch of the multiverse, by the MWI of the singlet state. So Mitra is right. Although Bertlmann's socks are tyically not working for Bell's violation in a MONO-universe, it works again in the MWI, applied in this case to the whole singlet state.

Bell has proved non-locality in MWI, every bit as much as in each branch separately. You appear not to have grasped the significance of the scenario I have argued carefully. Alice and Bob are not space-like separated in the scenario I outlined. Alice and Bob are together in the same laboratory when the second measurement is made. They are necessarily in the same world before, and branch in together according to Bob's result. Your mumbo-jumbo about them only being able to meet in appropriate matching branches does not work here, because they are always in the same branch. And there is no reason to suppose that their results in some of those branches do not violate conservation of angular momentum.

It's that last point I don't understand. Why isn't conservation of angular momentum a condition in every world. It's something separate from QM.

Yes, sorry, I seem to have got my negatives confused! There is no reason to suppose (in the time-like case proposed) that 'up-up' or 'down-down' combinations are impossible, and such combinations of results would violate conservation of angular momentum.

I'd say there is non-locality even when Bob's measurement is time-like because there is correlation with no physical causal link. The "common cause" of conserved angular momentum is not an explanation because that doesn't work in the space-like case and there's no reason to suppose QM is different in the two cases.

You are quite right here. The time-like and space-like separated measurements must give the same results, and have the same explanation. Common cause explanations don't work because space-like separations rule them out. My reason for considering time-like separation is that in that case one can precisely control the number of branches of the MWI involved, so that Alice and Bob are in the same branch when the crucial measurement is made. Thus there is no confusion over separate worlds that have to be matched up according to AM conservation when they finally meet -- they are always together, so there is no 'matching up' issue.

Bruce

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