On Friday, November 17, 2017 at 3:18:39 PM UTC-7, Bruce wrote:
>
> On 18/11/2017 12:10 am, Bruno Marchal wrote:
>
> On 15 Nov 2017, at 22:26, Bruce Kellett wrote:
>
> On 16/11/2017 1:55 am, Bruno Marchal wrote:
>
> On 15 Nov 2017, at 00:55, Bruce Kellett wrote:
>
> On 15/11/2017 12:47 am, Stathis Papaioannou wrote:
>
> On Mon, 13 Nov 2017 at 8:54 am, Bruce Kellett <bhke...@optusnet.com.au 
> <javascript:>> 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?
>
>
> I don't understand the significance of your question. Why wouldn't things 
> remain stable in MWI? After all, the whole world, as it is, becomes 
> entangled with the particular branching event.
>
>
> OK, but not instantaneously. This might be the point where we disagree in 
> the interpretation of the Non-collapse theory. 
>
>
> I think that the general idea is that the entanglement with the result 
> spreads at the velocity of light -- inside the forward light cone. This 
> spread of entanglement does not require that all objects in the forward 
> light cone have explicitly interacted with the original event. The 
> mathematics are quite clear on this point.
>
>
> You are right. So you might need an experience like Mandel & Co(I will 
> look at the reference, I guess you see which experience I allude to) where 
> two distant lasers create a singlet state non locally. That one has made me 
> doubt that MW could avoid Action-at-a-distance, and some thought experience 
> by Lucien Hardy too, but eventually, I remain unconvinced,
>
>
> You will have to give more precise references. Searching on these names 
> throws up so many papers that it is impossible to sort out exactly what you 
> mean here.
>
> because wherever are the actors, the singlet state never describes a 
> non-local affair, it only predicts the result of the people who will met at 
> some time.
>
>
> The singlet state is intrinsically non-local.
>

But as Brent claims, and I think he is correct, there is a basis in which 
the singlet state is a eigenfunction. In that basis, the obvious non 
locality may not be so obvious, if indeed it exists. AG
 

> It actually has nothing to do with whether people meet or not - it 
> describes a situation which explicitly violates Einstein's notion of local 
> realism: the state of one of the entangled pair is not separable from the 
> state of the other distant particle. Non-separability here implies 
> non-local influence, or simple non-locality. The attempt to claim that 
> non-separability does not imply non-locality is mere verbal gymnastics, 
> with no physical content.
>
> Bruce
>
>

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