On Sunday, April 22, 2018 at 4:19:44 PM UTC, Bruno Marchal wrote:
>
>
> On 20 Apr 2018, at 03:18, Bruce Kellett <[email protected] 
> <javascript:>> wrote:
>
> From: Bruno Marchal <[email protected] <javascript:>>
>
> On 18 Apr 2018, at 15:45, Bruce Kellett < <javascript:>
> [email protected] <javascript:>> wrote:
>
> From: Bruno Marchal <[email protected] <javascript:>>
>
> On 17 Apr 2018, at 13:52, Bruce Kellett < <javascript:>
> [email protected] <javascript:>> 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>.
>
>
> Those are not generalized basis vectors: they are eigenfunctions of the 
> spin projection operator in a particular basis. The singlet state is not a 
> superposition of vectors from different bases.
>
>
> Did I say that?
>


*You wrote |minus> when you meant |dn>, thus confusing the issue of bases. 
AG *

>
>
>
> 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 !!!!!!!
>
>
> Merely pointing out your apparent lack of comprehension when you fail to 
> appreciate the difference between the eigenvectors of a particular operator 
> and the free choice of a basis for Hilbert space.
>
>
> You aggravante your case.
>
>
>
> 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).
>
>
> So what?
>
> 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.
>
>
> Sure, the choice of basis is irrelevant. It is just that some bases are 
> more useful than others. And there is no use at all in trying to use all 
> bases at once!
>
> (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.
>
>
> Well, you are wrong.
>
> 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.
>
>
> I think you believe in a world. How else do you go about your daily life? 
>
>
> Like in a dream. Like in any computations which get a high relative 
> probability. Of course you can call that worlds, but they have no 
> fundamental ontology. But please read my papers, or the old posts.
>
>
>
> Or are you like most mathematicians: believing in platonism at work, but 
> believing in nominalism the rest of the time?
>
>
> I am a scientist. I keep my belief for myself except those I put on the 
> table as hypotheses, and reason from that. I do that in theology, which is 
> not done frequently especially since 1500 years (but some have the right 
> spirit, like Spinoza, and many others less well known).
>
>
>
>
> 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.
>
>
> No, due to the fact that any any "world" in which they find themselves the 
> correlations indicate non-locality.
>
>
> Yes, but not any action at a distance. 
>

*What is the content of non locality if not action at a distance, 
particularly for space-like separated events? AG *

>
>
>
>
> What is the particular magic that you put in the mix to ensure that the 
> correct correlations emerge?
>
>
> Only QM, without collapse.
>
>
> That is truly magical, and you have no evidence for this whatsoever.
>
>
> It follows from both QM and Comp. If Alice and Bob are space-separated, I 
> cannot even makes sense of how you can measure correlations, given that 
> once they are separated, whatever result they got, will be shared with 
> different Alice and Bob in different branch. I am not even sure we can 
> define what could be an action at a distance in the quantum formalism. The 
> notion does not even makes sense when we assume special relativity. The 
> only reason to believe this is the habit to think that there is only one 
> bob and one Alice, which makes no sense once separated, unless they are 
> correlated with a third observer, but then, again by looking at the wave 
> without collapse, there will be no action at a distance. The no locality is 
> only an appearance due to the fact that we belong to infinities of 
> histories, and cannot known which one we are in.
>
> Bruno
>
>
>
>
> Bruce 
>
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