On Mon, 13 Nov 2017 at 8:54 am, Bruce Kellett <bhkell...@optusnet.com.au>
wrote:

>
> I don't think you have fully understood the scenario I have outlined.
> There is no collapse, many worlds is assumed throughout. Alice splits
> according to her measurement result. Both copies of Alice go to meet
> Bob, carrying the other particle of the original pair. Since they both
> have now met Bob, the split that Alice occasioned has now spread to
> entangle Bob as well as the rest of her environment. So there are now
> two worlds, each of which has a copy of Bob, and an Alice, who has a
> particular result. Locality says that Bob's particle is unchanged from
> production, so when he measure its spin, he splits into two copies,
> according to spin up or spin down. Since Alice is standing beside him,
> she also becomes entangled with his result. But Alice already has a
> definite result in each branch, so we now have four branches: with
> results 'up-up', 'up-down', 'down-up', and 'down-down'. However, only
> the 'up-down' and 'down-up' branches conserve angular momentum. How do
> you rule out the other branches?


When you put something in the cupboard and come back later to get it, why,
under MWI, is it still there?

> --
Stathis Papaioannou

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