On Thursday, August 16, 2018 at 10:05:31 AM UTC, Bruno Marchal wrote:
>
>
> On 15 Aug 2018, at 13:33, Bruce Kellett <[email protected] 
> <javascript:>> wrote:
>
> From: Bruno Marchal <[email protected] <javascript:>>
>
> On 15 Aug 2018, at 01:48, Bruce Kellett <[email protected] 
> <javascript:>> wrote:
>
> From: Bruno Marchal <[email protected] <javascript:>>
>
> On 14 Aug 2018, at 04:30, Bruce Kellett <[email protected] 
> <javascript:>> wrote:
>
> If they are space separated, I am not sure I can make sense of being in 
> the same branch. 
>
>
> You appear to be referring to the presence of quantum fluctuations 
> continually splitting the classical Alice and Bob into multiple copies -- 
> the point that Jason has made.
>
>
> That points is correct, but I was alluding to the infinity of Bob and 
> Alice couples associated with the singlet state. That is needed to tackle 
> the case where Alice and Bob makes non orthogonal measurements.
>
>
> I was trying to make sense of the suggestion of many Alices and Bobs 
> before any measurement. That can easily be implemented by having  Alice 
> select her measurement angle according to the time of some radioactive 
> decay. Since an infinity of decay times is possible, we get a superposition 
> of an infinite number of copies of Alice. 
>
>
> OK. But we have this in our context too.
>
> But this makes not difference to the basic argument -- one just picks out 
> a typical Alice. 
>
>
> How?
>
>
> Do you really no know how to pick out a typical component from an ensemble?
>
>
>
> I cannot when the elements cannot be distinguished. Alice cannot do that, 
> but each Bob and Alice picks their counterparts by doing their 
> measurements, but that take some times.
>
>
>
>
> You are wrong when you claim that an infinity of couples are required to 
> make sense of measurements made at arbitrary angles.
>
>
> Why?
>
>
> Because that is not how angular momentum operators in quantum mechanics 
> work.
>
> The singlet state is rotationally symmetric, 
>
>
> That’s why.
>
>
> That's why what?
>
>
>
> That is why a singlet state describe a collection of situations 
> withAlice’s particles spin well defined in all directions (and the opposite 
> for Bob). But none know which one.
>
>
>
> and can be expressed in any base. But this does not mean that there 
> actually exists a copy of the observer for each of the potential bases. 
> That idea makes no sense at all; it is not part of quantum mechanics in any 
> possible formulation.
>
>
> ?
>
> That would contradict the complementary principle. A well localised 
> particle is a particle having almost all possible momenta in many different 
> histories.
>
>
> For fuck's sake, Bruno. Do you understand nothing of elementary quantum 
> mechanics?
>
>
> No comment.
>
>
>
>
> The angular momentum operators do not commute, sure, so that if one has a 
> precise measurement in one direction, one has no knowledge of the 
> projection in an orthogonal direction. But the possible values of any such 
> operator on the spin-1/2 state are +1 or -1 (in units of hbar/2). So there 
> is no infinity as there is in the case of the complementarity of position 
> and momentum operators!
>
>
> No problem with this, but Alice can choose to measure that spin in any 
> direction.
>
>
>
>
> Besides, it is possible to have exact values for both the total angular 
> momentum operator (L^2) and any particular component, say L_z if we are 
> measuring in that direction, and that is all we require here. See the 
> Wikipedia article:
>
>
> https://en.wikipedia.org/wiki/Angular_momentum_operator#Uncertainty_principle
>
>
> The singlet state does not single out one base, despite the notation. It 
> describes an infinite of Alice and Bob right at the start.
>
>
> Sure, the singlet state does not single out one base. But that does not 
> mean that it describes an infinity of observers. Just because you can 
> measure at any angle does not mean that there is actually an infinity of 
> observers making all those possible measurements. That notion is just crazy.
>
>
> ?
>
> It is just what the wave described literally. 
>
>
> No, it is not. Look up some reference on the application of the 
> uncertainty principle to angular momentum operators. (Such as the Wikipedia 
> article above.)
>
>
> I do not see any problem between what I said and that wiki pages, which is 
> rather neutral on the interpretations. They do not provide the 
> “many-worlds” view on this, and some links there suggests they use the 
>  Copenhagen formulation. 
>
> You seem to reintroduce implicitly some collapse in the picture. That’s my 
> feeling, as this is not clear. When measuring a spin: there are two 
> possible values *for all possible direction of the spin*. That makes 
> infinitely many worlds. Same for an electronic orbital. There are as many 
> world that the possible position of the  electron in the orbitals.
>


*In such scenario, you'd have to include all bound electrons in the 
universe, bound to atoms and molecules, from which the number of possible 
worlds and Alice's would hugely metastasize. I am fine with this scenario 
provided you add immaculate conception to the multiple universes and 
Alice's. AG *

> Are you OK with this? I try to figure out what is your interpretation of 
> the SWE.
>
> Bruno
>
>
>
>
>
> Bruce
>
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