> On 2 Aug 2018, at 01:32, Bruce Kellett <[email protected]> wrote:
> 
> From: Bruno Marchal <[email protected] <mailto:[email protected]>>
>>> On 1 Aug 2018, at 06:19, Bruce Kellett <[email protected] 
>>> <mailto:[email protected]>> wrote:
>>> 
>>> 
>>> No, there are not any infinities of anything. You simply confuse yourself 
>>> by continuing to claim such things which are not part of quantum mechanics.
>> 
>> 
>>  The singlet state just means that They will see correlated result when 
>> coming back together. Let me put it in this way: if Alice and Bob are space 
>> separated, I do not see how to give meaning to “to be in the same branche”, 
>> and they might individually get non correlated spin measurement?
> 
> It is easy to see how they can be in the same branch, even if space-like 
> separated. I gave an account of how all measurements are made in the same 
> branch by starting with the time when Alice and Bob meet to compare notes 
> after their series of experiments and working backwards to show that, since 
> neither can jump between branches, all measurements must have been made in 
> the same branch.
> 
> You can do the same thing in the forwards time direction by considering that 
> the singlet is prepared in one world.

I cannot make sense of this. Preparing a singlet state is typically done in an 
infinity of “worlds” (or some very big numbers of worlds in some version of 
quantum gravity, but for simplicity I assume just “classical” QM). 

I have to go. Will read the sequel later. But it seems to me that you 
constantly postulate a collapse. The notion of singlet state is typically a 
many-world construction, even in Copenhagen before the "measurement/collapse”. 

Bruno





> The component particles move off in separate directions, but they can't jump 
> worlds either, so when Bob gets his particle to measure, he is necessarily in 
> the same world as that in which Alice makes her measurement -- the singlet 
> state itself guarantees that. Then they make their measurements: each gets 
> either up or down, so each splits into two branches. But the branch with, 
> say, Alice_up is connected with the original branch in which Bob sits. He 
> splits into two branches on measurement, but again, each branch is connected 
> with the original Alice branches. There are now four branches: 
> Alice_up-Bob_up, and so on for the other combinations. Each of these branches 
> defines a single world in which there are a pair of measurements. And, 
> because of the way in which these branches are always interconnected, the 
> results of each experimenter, if repeated many times, will always have the 
> correct quantum correlations. There are no other branches -- and no 
> unconnected measurements that have, somehow, to be discarded -- they can 
> never get uncorrelated spin measurements! 
> 
> 
>> Bell’s inequality will not been violated, because that Bob and Alice will 
>> never meet again. Each of them will meet only their relevant counterparts 
>> when they will “meet again”. 
>> 
>>>> and all what they both know is that they share some historical reality 
>>>> with a relative partner, so that their simps are correlated, but they are 
>>>> are ignorant and thus distributed on infinitely many histories, with all 
>>>> the correlation between different spin “angle” (assuming a fixed base to 
>>>> describe them).
>>>> I might be wrong, but the violation of Bell’s inequality (or 
>>>> Kochen-Specker theorem) does not entail any physical instantaneous action 
>>>> at a distance. I have seen may attempt to prove this, but they always 
>>>> favour a branch in a way or another, forgetting the probabilities bear on 
>>>> different portioning of the multiverse in the big picture. 
>>> 
>>> Any evaluation of a set of correlations between experimental results 
>>> happens in one branch of the superposition. So much for "favouring a branch 
>>> in a way or another." There is simply no other way to evaluate the 
>>> correlations. There is no "big picture" that is going to change this 
>>> conclusion.
>> 
>> Then you assume some collapse.
> 
> As usual, that is your fantasy (i.e., a meaningless bolt-hole by which to 
> escape an inevitable mathematical conclusion). No collapse is assumed.
> 
>>>> It makes the whole physics becoming covariant, despite necessary relative 
>>>> local appearance of what seem to be an action at a distance. There are 
>>>> none, but to show this, we must take into account the fact that Alice and 
>>>> Bob find all correlated results in all directions.
>>> 
>>> Physics is covariant in any case. The non-locality is real -- it is not 
>>> just an 'appearance'. Bell's theorem and the observed correlations prove 
>>> this.
>> 
>> I don’t see this. The violation of Bell’s inequality is real, but without 
>> any collapse, all interactions are local, and spread locally fro the place 
>> where they have been done. That follows from the wave only, and that 
>> guaranties that Alice and Bob, when coming back, will see the 
>> correlation/violation, but Alice and Bob does that only with some relative 
>> counterpart of Bob and counterpart of Alice respectively. 
> 
> You keep returning to this idea of a "common cause" explanation. And that, as 
> we know, is ruled out by Bell's theorem. And all attempts to undermine Bell's 
> theorem end in disaster -- Bell's theorem is called a theorem for good reason.
> 
>> Like Maudlin says: “Or finally once can both avoid collapses and retain 
>> locality by embracing the Many-Minds ontology, exacting a high price from 
>> common sense”.
> 
> That refers directly to the "many-minds" interpretation of QM. And Maudlin, 
> as well as everyone else, has long since moved on from this position. You 
> should go to the library and read the third edition of Maudlin's book for his 
> more recent position.
> 
> Bruce
> 
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