On Monday, June 11, 2018 at 1:37:53 AM UTC, Bruce wrote:
>
> From: Bruno Marchal <[email protected] <javascript:>
>
> On 8 Jun 2018, at 14:55, Bruce Kellett < <javascript:>
> [email protected] <javascript:>> wrote:
>
> From: Bruno Marchal <[email protected] <javascript:>>
>
> On 8 Jun 2018, at 02:32, Bruce Kellett < <javascript:>
> [email protected] <javascript:>> wrote:
>
>
> The SWE does not give a preferred basis. Basing MWI on the Schrödinger 
> equation runs into the basis problem. Few MWI advocates actually take this 
> seriously. And they should.
>
>
> The relative proportion of histories do not depend on the choice of the 
> base, so the base we use are chosen endemically, like the present moment 
> for example, in the whole of physics. Obviously, we needs brain to assess 
> our results and communicating, and some works, like sure and others, 
> justify the indexical importance of the position base, with respect to the 
> branch where intelligence can develop.
>
>
> What on earth are you talking about? The position basis is not 
> well-defined either. The Hilbert space corresponding to the position 
> operator X has an infinite number of possible bases -- just like any other 
> Hilbert space. Any linear vector space has an infinite number of possible 
> bases. How do you choose which one you are going to use? Talking about the 
> relative proportion of histories sounds just like the long-since refuted 
> branch counting approach to probabilities. 
>
>
> Measure is quite different from counting.
>
>
> And the probabilities for various outcomes most certainly depend on the 
> chosen base, as do the outcomes themselves.
>
>
> Well, we can use what we call in French “le peigne de Dirac”. To make that 
> precise Laurent Schwartz has invented the theory of distribution. I 
> simplify things here. Consider that space has been quantised, like in 
> Loop-Gravity or something. Here, you do a 1004 fallacy, with respect to the 
> goal (helping Grayson to have an idea of what is QM-without-collapse).
>
>
> ?
>
>
> * In this situation, what is the role of the SWE since the wf is usually 
> asserted without any reference to it? Now consider a general case where the 
> wf for a system is determined using the SWE. Since the solution can be 
> expanded using difference bases, say E or p, does each possible expansion, 
> each implying a different possible set of measurements, imply a different 
> set of worlds using the SWE? TIA, AG*
>
>
> The Schrödinger equation merely gives the time evolution of the system. To 
> define the problem you have to specify a wave function. It is in the 
> expansion of this wave function in terms of a set of possible eigenvalues 
> that the preferred basis problem arises. So it is not really down to the SE 
> itself, it is a matter for the wave function. Each expansion basis defines 
> a set of worlds, and all bases give different worlds.
>
>
> That is correct, but the choice of the basis don’t change the relative 
> “proportion of histories”.
>
>
> The choice of basis makes all the difference in the world. 
>
>
> Everett prove the contrary, and he convinced me when I read it. I found 
> “his proof” used in many books on quantum computing, although with 
> different motivation. Thee result of an experiment, obviously depend of 
> what you measure, but when you embed the observer in the wave, you get that 
> what they find is independent of the choice of the base used to describe 
> the “observer” and the “observed”. If not, the MW would already be refuted.
>
>
> In that case, MW is refuted. Clearly, what the observer finds is dependent 
> on the basis in which he is described. Or else experiments would not have 
> definite results when described in the laboratory from the 1p perspective. 
> Even if you take the 'bird' view of the whole multiverse -- which is, I 
> agree, independent of the basis in which it is described -- the view of any 
> observer embedded in the multiverse is totally basis-dependent. That is, 
> after all, what we mean by 'worlds' -- the view from within, or the 1p 
> view. But that view depends on how you describe it: the way in which you 
> partition the multiverse itself. Only certain very special bases are robust 
> against environmental decoherence -- how else do you resolve the 
> Schrödinger cat issue?
>
> Bruce
>

*So you find the resolution in the fact that according to decoherence 
theory, the cat is simultaneously alive and dead for only short time?  AG*

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