On Fri, Nov 24, 2017 at 1:15 PM, Bruno Marchal <[email protected]> wrote:

>
>
> I was just explaining that a measurement is any memorable interaction,
> which is simplest to illustrate with a tensor product of Alice (|A>)and a
> simple superposition. In your notation: |A> (|UP> + |DN>) = |A> |UP>  + |A>
> |DN> .
>
> In the case of the singlet state, it is more subtle, as  |UP>|DN> -
> |DN>|UP> describes a many-worlds with Alice having a spin in any direction,
> and Bob, too but the opposite relatively to each others (the notation is
> misleading). We must keep in mind the rotational invariance of the spin. So
> we the Alice Bob situation is more intricate and tedious to describe.
> Sometimes I referred to the simple account of this in the Everett FAQ by
> Michael Clive Price, but it seems not available since some times. We have
> copied the relevant details in previous discussions though, so you might
> try to find it in the archives with the key word "Michael", or something. I
> have unfortunately not the time "here and now".  Later perhaps. With
> Everett, it is important to reason independently of the bases in between
> the measurements.
>
> I guess you see that violation of the BI leads to "action at a distance"
> if we assume a collapse, or a mono-world theory.  I don't see Bell'
> argument applying in the MW context, though.
>
> Bruno
>
>
>
Bruno,

Is this the Many Worlds FAQ you were referring to?
http://www.anthropic-principle.com/preprints/manyworlds.html

I think the parts relevant to EPR, Bell Inequality and Locality (for those
interested) are Q12 and Q32.

Jason

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