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Sherlock
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Each of the two views depends on an, imo, unfounded interpretation of the meaning of quantum theory. The relationship between the theoretical unitary evolution and the evolution of quantum systems in real, 3D space is just not known.ttn said:We've been around on this so many times here, I'm already dizzy. So I'll make a few comments, and then give you the last word. Then we can let other people assess the two views and decide for themselves.
What I believe is that quantum theory provides one way (so far, apparently, the best way) of calculating the average results of large numbers of identically prepared experiments on quantum systems. Beyond that, any meaning that I attach to the formalism is, for the moment at least, purely speculative.
The Bell locality condition isn't necessarily an evaluator of locality vs. nonlocality. Disagreement with this condition does indicate that the statistics of spatially separated detectors are not independent, that they are related. But this doesn't necessarily mean causal dependence due to some sort of superluminal transfer between the filters or detectors during measurement intervals. There is, imo, a better way to approach understanding how the correlations can occur in a universe where all propagations are limited by the speed of light.
Nevertheless, nonlocality in nature remains an interesting possibility. But, I don't think that the same can be said for MWI.
ttn said:If it weren't for the claim that MWI saved locality, I submit that *nobody* would take MWI even remotely seriously. It's just too stupid/crazy/la-la-land to even consider *science* unless there's some very powerful argument in its favor. I concede that saving locality is in the ballpark of such an answer. But I still come down on the side of saying: the price is *way* too high.
Locality doesn't really need to be saved, because the inference of non-locality depends on an interpretation. If there was actually any physical evidence of non-locality, then there wouldn't be any talk about saving locality. There would be a joyous reworking of physics to incorporate this wonderful new phenomenon that would be embraced by all physicists.
iiuc, the relative-state interpretation was forwarded by Everett to deal with what some see as an inconsistency between the theoretical evolution of the wavefunctions representing the possible results of an individual measurement, and the directly observed fact that only one of these possibilities is actually produced per individual measurement.
Why that's a problem, I don't know.
To make reality fit their interpretation of the meaning and application of quantum theory, the MWIers invent as many worlds (branches of reality) as needed to accommodate the possible results of measurements. This is, to me, obviously a perversion of the meaning and application of quantum theory, and goes against the basic tenet of empirical science.
So, I agree with you, ttn, wrt your assessment of and objections to MWI. But, I disagree with your interpretation of the meaning of quantum theory insofar as you hold that it implies non-locality in nature. I'm somewhat surprised that vanesch has adopted the MWI approach. And, I'm sorry to disagree with either of you on anything, because you have been very good teachers, but wrt this matter I must ... until otherwise corrected.
To summarize, there is no definitive interpretation of the physical meaning of quantum theory beyond its obvious role as a method of calculating experimental results. There is no locality problem. There is no wavefunction collapse problem. There is of course a real measurement problem, but it has to do with what can be experimentally determined rather than some pseudo-difficulty arising from unnecessary interpretations of the formalism.
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