Re: Multiverse Morality
Gary Oberbrunner <[email protected]> Wed, 28 Aug 2013 19:52:55 -0400
| Newsgroups | gmane.science.physics.fabric-of-reality |
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| Message-ID | <CAFChFyjA4a9ys32UFxSSQi9F824VYHPr5oVzCXuf99JGCdT=cg@mail.gmail.com> |
[My gmail seems to sometimes produce bad indentation --I'll write this one in Emacs.] On Wed, Aug 28, 2013 at 6:22 PM, hibbsa <hibbsa-/[email protected]> wrote: ... > On that matter - the tense that you are raising here with your chaos > example of macroscopic amplification - my basic position has been > that I am saying exactly the same thing that MWI itself > says. Namely, that the multiverse represents all the possible > outcomes, in the same way that, within a one-universe model - a > statistical model of the possibilities would say the same thing. As > such, the multiverse could be conceptualized as a statistical > model. Albeit one that cannot be derived for real. You have it just right; [quantum] probability in the single universe we see is the same as measure in the multiverse. I'd only say that the multiverse *can* in fact be derived for real; that derivation is a straightforward application of the SWE. > In that context, what I am challenging, is whether the multiverse - > in context of the divergence from some ancestor world, can ever > produce novelty that, were that novelty to have occurred in the > ancestor world, it would have amounted to a statistically > significant change in that ancestor world. OK, let's unpack that. We have an ancestor world A. (By "world" I presume we're talking about a bounded region of spacetime.) It produces several successors: B, C, D, and so on. (Note that the time bounds of these are later than A's time bounds, otherwise A wouldn't be their ancestor.) Let's take B, which we know to be quite different from A. I think what you're saying is C, D and the others are very much like each other, but B is different (it has "diverged" macroscopically from its siblings). Of course none of them are much like A, since they're all later and things have presumably changed over time. So the multiverse produced novelty in the form of B. So far, so good. Can you walk through the counterfactual part ("were that novelty to have occurred...") in this example? Are you asking how that novelty could get from B (a small fraction of worlds) to become a large fraction of worlds later on, so, say, the grandchildren of B would come to dominate over the grandchildren of C, D, etc.? Or something different? Feel free to rework my example to show your point. > But the problem I have with applying that sort of theory within the > context of emergence, is that....what if there are 100 or 100 fully > distinct emergent levels in our universe. I disagree with this. I think each concept (entropy, intelligence, macroscopic objects, etc.) has its own emergent properties and layers of emergence, and they're quite fuzzy; there's no way to slice that across all concepts so there are 100 "fully distinct emergent levels". > So far as I know, there are no properly worked through variants on > chaos theory, that describe the effect in terms of that emergence. This could be a good area for research perhaps? Chaos theory itself is quite well researched and worked through mathematically. Modern communication theory for instance would be impossible without detailed models of chaotic behavior. And of course chaotic behavior is strongly emergent; fractals are the obvious example, but so is period-doubling and various kinds of attractors. But I'm sure there's more to be figured out. > I don't even think there are yet any hard scientific models of > emergence that have made it all the way to mathematics. Isn't that exactly what thermodynamics is? A model of how quantum random behavior leads to stable (emergent) chemistry and physics? And on the intelligent-behavior-emergence front, there's a lot of a-life work that could be seen as relevant (producing "intelligent" behavior by evolving random genotypes for instance -- there's a lot of work done around that kind of thing.) > In which case, it's hard to see how it can currently be regarded as > reliable, robust, reasoning, to speak of such effects within a > context of emergence at all. You may have something different in mind from standard emergent properties here. > Beyond that, as I mentioned to you in a private mail a few weeks or > months back, the issue I am raising here is not primarily about MWI > itself, but about Deutsch's specific variant of MWI, which heavily > involves the concept of fungibility. Emergence isn't directly > linked, but he does describe a personal theory about emergence in > BoI. So the issue I'm raising is really about whether these three > concepts all work together properly, or whether there is a problem. > For example, can you or anyone, explain how worlds can be fungible - > which Deutsch describles as being literally in the same dimensional > 'place' Well, I don't know about Deutsch (I can't make it through BoI, it's too loosely argued) but fungibility is quite a standard term in physics. It just means completely indistinguishable. Two photons are fungible if they can be swapped without any effect. In the MWI, an Electron which can be spin-up or spin-down has an infinite (or at least huge) number of spin-up little-e electrons and the same number (really equal measure) of spin-down little-e electrons. All the spin-up ones are fungible with each other, all the spin-down ones are fungible with each other, but the spin-up ones have a different property from the spin-down ones so they are not fungible with each other. The canonical example is a Bose-Einstein condensate. Google that for more. Macroscopically I think the concept of fungibility gets fuzzier, but it's certainly possible to say "...in all the worlds in which I do the Schroedinger's Cat experiment..." and mean that all those worlds, which may be microscopically variant, are FAPP fungible up to the point of the photon being emitted (in some of them). There's no real difference between them, you can't tell which one you're in, they all have the cat, the vial, the experimenter, etc. But of course that macroscopic "FAPP" fungibility doesn't mean literally fungible in the QM sense. Of course there are many macroscopic fully-fungible regions of spacetime, but at the macro level physicists usually don't care about where particular air molecules are. It's another form of emergence I guess: what counts as fungible depends on the question. (Just like two dollar bills are fungible when considering their value, but not when considering their history, pattern of folds, or serial numbers.) > ....and not just at the quantum level but at all levels. How > does that work, using Deutsch's description of emergence which > explicitly rejects a purely bottom-up determinism in terms of > emergences. > The implication being, that macroscopic levels - supposedly fungible > - can potentially be influenced by top-down effects, which > presumably in some possible instances result in changes at the > macroscopic level. Which presumably would violate fungibility. Which > so far as I can see, would have to be see as a refutation of the > concept of fungibility itself, unless Deutsch has an explanation how > this can nevcer happen.....which in turn maintains consistency with > his explanation of emergence itself. I'm afraid I get lost in these last two paragraphs -- I'd need to understand Deutsch's concepts better I guess. -- Gary [Non-text portions of this message have been removed]