On Thursday, April 19, 2018 at 10:11:38 PM UTC, smitra wrote:
>
> On 19-04-2018 22:52, [email protected] <javascript:> wrote: 
> > On Thursday, April 19, 2018 at 2:42:37 PM UTC, Bruno Marchal wrote: 
> > 
> >> On 18 Apr 2018, at 15:45, Bruce Kellett <[email protected]> 
> >> wrote: 
> >> 
> >> From: BRUNO MARCHAL <[email protected]> 
> >> 
> >> On 17 Apr 2018, at 13:52, Bruce Kellett <[email protected]> 
> >> wrote 
> >> 
> >> But note particularly that the spin measurement is made in the 
> >> basis chosen by the experimenter (by orienting his/her magnet). 
> >> 
> >> OK. 
> >> 
> >> The outcome of the measurement is + or -, 
> >> 
> >> For Alice and Bob, OK. 
> >> 
> >> not one of the possible infinite set of possible basis vector 
> >> orientations. The orientation is not measured, it is chose by the 
> >> experimenter. So that is one potential source of an infinite set of 
> >> worlds eliminated right away. The singlet is a superposition of two 
> >> states, + and -: it is not a superposition of possible basis 
> >> vectors. 
> >> 
> >> ? (That is far too ambiguous). 
> > 
> >  ????? It is not in the least ambiguous. The singlet state is not a 
> > superposition of basis vectors. 
> > 
> > ? 
> > 
> > The singlet state is the superposition of Iup>IMinus> and (Minus>Iup>. 
> > 
> >> If you think about it for a little, the formalism of QM does not 
> >> allow the state to be written in any way that could suggest that. 
> >> 
> >> I don't know what Everett says in his long text, but if it is any 
> >> different from the above, then it is not standard quantum mechanics. 
> >> Deutsch is a different case. He has a very strange notion about what 
> >> constitutes different worlds in QM. Standard QM and Everett's 
> >> interpretation are very clear: different worlds arise by the process 
> >> of decoherence which diagonalizes the density matrix. The net effect 
> >> is that worlds are, by definition, non interacting (contra Deutsch's 
> >> ideas). 
> >> 
> >> ? 
> > 
> >  This relates to your lack of comprehension above. 
> > 
> > Patronising !!!!!!! 
> > 
> >> Deutsch has two distinct notions of "world" in his approach. He has 
> >> the standard Everettian notion of a "relative state" corresponding 
> >> to each term in the superposition of possible measurement outcomes. 
> >> These relative states are made definite by decoherence, 
> > 
> > Relatively. Decoherence is only entanglement (with NON-collapse). 
> > 
> >> and then correspond to different, effectively orthogonal, worlds, 
> >> each of which represents the experimenter observing one particular 
> >> result. But Deutsch also has the idea that the infinity of possible 
> >> bases for an unpolarized qubit also represents an infinity of 
> >> worlds. 
> > 
> > That is necessary, and Everett explains this well when he shows that 
> > the choice of the base to describe the universal wave is irrelevant. 
> > 
> > (A bit like the choice of the universal Turing formalism is irrelevant 
> > to get the theology and the physics). 
> > 
> >> This is quite a different notion, and does not occur in Everettian 
> >> theory. 
> > 
> > I disagree with this. 
> > 
> >> In this second notion of "world", the worlds remain in 
> >> superposition and continue to interfere -- there is no separation 
> >> into disjoint, non-interacting worlds. In fact, it is precisely this 
> >> continued interference of these supposed "worlds" that is the 
> >> explanation for the action of quantum computers -- which Deutsch 
> >> seems to think actually *prove* his notion of quantum "many-worlds". 
> >> He is out on a limb on this one, and few experts, even in the 
> >> quantum computing field, agree with Deutsch on this new notion of 
> >> "worlds". The essential continued interference between the different 
> >> basis states in fact means that the "worlds" remain inextricable 
> >> "one world". (See some of Scott Aaronson's comments on Deutsch and 
> >> many-worlds in his lecture notes on quantum computing.) 
> >> 
> >> So when you continue to refer to an "infinity of worlds" for the 
> >> measurements on the entangled spin states, you are using a notion of 
> >> "world" that does not occur in Everett, and is inherently 
> >> controversial, if not entirely meaningless. 
> > 
> > I use the “Herbrand” interpretation of quantum mechanics without 
> > collapse. I mean: it is literal QM (in a sense that logicians have 
> > made precise) without collapse up to a choice of any arbitrary base. 
> > I don’t believe in any worlds, to be clear. It always means some 
> > reality satisfying some formal constraints. 
> > 
> >> But even if you can manufacture an infinity of universes, you still 
> >> have not shown how this removes the non-locality inherent in the 
> >> quantum formalism. 
> >> 
> >> You have not shown non locality. 
> > 
> >  I have demonstrated non-locality in the Everettian context many 
> > times. The simplest demonstration was in the timelike separation of 
> > Alice and Bob's measurements. It is in the archives if you don't 
> > recall the details. The argument then is that any local influence that 
> > would explain the timelike separated measurements must also work for 
> > spacelike separated measurements, and that is not possible. 
> > 
> > At all time there is an infinity of “worlds”. When Alice chose her 
> > direction, that remains true, and her measurement will tell us if she 
> > belongs to a world with “spin” down or up, she will automatically 
> > know that whatever Bob she will meet, will have the corresponding 
> > results, no action at a distance here. 
> >  Again, you keep referring to this non-existent infinity of worlds — 
> > 
> > 
> > “worlds” would be better. 
> > 
> >> a notion that has nothing to do with Everett or his interpretation 
> >> of quantum theory. "... She will automatically know that whatever 
> >> Bob she will meet, will have the corresponding results...". This is 
> >> precisely the question that you have not answered -- how does this 
> >> happen? 
> > 
> > Because in ALL “worlds” Alice and Bob have they spin described by 
> > the no-separable singlet state. The statistics seems non-local, due to 
> > their ignorance of which partition of the wave function they belong 
> > to. 
> > 
> > But that would be the same for all worlds; statistics which imply 
> > instantaneous action at a distance. You haven't removed non-locality, 
> > but in fact extended it to many worlds, and then you must ignore the 
> > elephant in the room; the absurdity of postulating the many observers 
> > with identical memories, histories, etc. I don't see that anything has 
> > been gained. AG 
>
> The non-locality is eliminated here via a common cause effect. But the 
> common cause explanation only works if you don't get rid of the 
> superposition that includes sectors where Alice and Bob find different 
> results. 
>
> Saibal 
>

Sorry. I don't follow your comments. Bruno claimed the statistics in all 
worlds
imply non-locality.  AG

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