On Thursday, August 23, 2018 at 3:16:24 PM UTC, Bruno Marchal wrote:
>
>
> On 23 Aug 2018, at 02:05, Bruce Kellett <[email protected] 
> <javascript:>> wrote:
>
> From: Bruno Marchal <[email protected] <javascript:>
>
> On 22 Aug 2018, at 01:54, Bruce Kellett <[email protected] 
> <javascript:>> wrote:
>
> From: Bruno Marchal <[email protected] <javascript:>>
>
> The other sort of infinity, the one which I think you disagree with, is 
> typical for the  superposition of tensor products, like the singlet state 
> ud - du. Before measurement Alice has the same probability of finding u, or 
> d for any measurement she can do in any direction. Both Alice and Bob are 
> maximally ignorant of their possible measurement results. The MW on this, 
> or a MW way to interpret this, to keep the rotational symmetry, is that we 
> have an infinity of couples Alice+Bob, with each couple being correlated.  
> If not, some implicit assumption is made on u and d, like it is a preferred 
> base.
>
>
> But the problems with any such suggestion are obvious. Firstly, Alice does 
> not choose her measurement angle in that way, so there is no 
> super-superposition created. Secondly, this construction does not restore 
> the rotational symmetry in any case. You might have an infinite number of 
> Alices, measuring the singlet at all possible angles, but that 
> multi-multiverse is not rotationally symmetric either! All it needs is for 
> Alice number 7,234,826 to poke her tongue out and the rotational symmetry 
> is lost! Of course, you could add yet more multiverses to cover every 
> possible deviation of Alice from the stationary state. But the process 
> rapidly becomes ridiculous.
>
> So this Rube Goldberg construction of additional multiverses of 
> superpositions does not actually restore stable rotational symmetry. So why 
> propose such a construction? William of Ockham will rise out of his grave 
> to haunt you for such pointless extravagance of entities!
>
>
> Alice destroys the rotational symmetry in all its universe. Not of the 
> whole wave, where Alice does not exist as a determinate subsystem.
>
>
> I can't really parse this. The point is that when Alice interacts with the 
> singlet with her magnet she destroys the rotational symmetry of the state. 
> This symmetry is not restored by considering and large system, or the whole 
> wave. If anything, enlarging the context in this way simply lessens any 
> symmetry that might remain.
>
> I think what you have in mind is a situation such as arises if you shine a 
> light through a small aperture. The photon emerges as a spherical wave, 
> with the rotational symmetry of such a (hemi-)spherical wave. If there is a 
> hemispherical screen downstream, the photon will interact with the screen 
> at some single point. If you consider only one branch of the SWE evolution, 
> this interaction point breaks the rotational symmetry. But if you consider 
> all branches of the wave function together, there is a branch for every 
> single point at which the photon can hit the screen, so that the symmetry 
> is preserved in the wave function as a whole -- over the ensemble of all 
> branches. But that is a situation in which the environment with which the 
> photon interacts is itself symmetrical. If the screen, rather than being a 
> smooth equidistant hemisphere, is just the rough walls of the laboratory, 
> there is no symmetry in the points at which the photon can hit the walls, 
> and the rotational symmetry is lost, even in the wave function as a whole, 
> even by considering the superposition of all possible branches.
>
> The take away message from this is that the symmetry of the original 
> system can be lost by interaction with a non-symmetrical environment. The 
> boundary conditions of the total system may not have the symmetries of the 
> original state. So loss of symmetry is ubiquitous in the universe, even for 
> Everettian no-collapse quantum mechanics. If you introduce a 
> non-symmetrical interaction into the system, the symmetry is lost. That is 
> all that is happening with the measurement of the spin projection of the 
> singlet state by Alice. Your idiosyncratic interpretation of the tensor 
> product, and your insistence the the symmetry be preserved regardless of 
> the non-symmetrical environment, are just misguided. There is no need to 
> try to preserve symmetry given non-symmetrical boundary conditions.
>
> Since the symmetry is broken, the singlet state no longer exists in its 
> original form, and the state that Bob measured is affected by the 
> measurement Alice makes. There is no more to it than this. If Alice and Bob 
> are space-like separated, there are some interpretational issues with this 
> instantaneous influence at a distance.
>
>
> Nice to hear that. It was basically my point.We have never disagreed 
> except on some definition. I use “symmetry” in a larger sense, and I take 
> superposition at face value, independently of the base, making the 
> superposition of tensor products into “many superposition”, which indicate 
> the relative state locally accessible by the observers.
>
>
>
> But that just means that quantum mechanics is not fully integrated with a 
> total quantum theory of space-time.
>
>
> Yes.
>
>
> No need to get agitated by this -- ride with it until we have a more 
> complete theory. In the meantime, this is what is meant by non-locality.
>
>
> It means violation of Bell’s inequality. I get agitated only by those 
> implying the existence of instantaneous physical action at a distance, 
> that’s all.
>
> Bruno
>

*But keep in mind that if the wf is epistemic only, it can change 
instantaneously with no PHYSICAL action at a distance. This is what Bruce's 
horse race example shows, and FWIW, my present assessment of the situation; 
wf epistemic only. AG *

>
>
>
>
> Bruce
>
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