For the bus ride home, I'm going to check out "One world versus many: the inadequacy of Everettian accounts of evolution, probability, and scientific confirmation" by Adrian Kent (arXiv/0905.0624) Nothing like ending the day with some against many-worlds reading. That and a fun TED talk should make the ride go by fast
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I think I missed this the first time around, but this weekend, I watched the bloggingheads conversation about quantum mechanics between Sean Carroll and David Albert. In it, David makes an extended argument against the Many-Worlds Interpretation of quantum mechanics (starting about 40:00 into the…
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Last week's post about the Many-Worlds variant in "Divided by Infinity" prompted the usual vigorous discussion about the merits of the Many-Worlds Interpretation. This included the common objection that we don't know how to obtain the probability of measurement outcomes in the Many-Worlds…
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I've seen Adrian talk about this stuff and I think it will be a good paper. For the proper context, it needs to be read in conjunction with David Wallace's papers on probability in many-worlds.
One thing that struck me about most every approach to no-collapse interpretations, including this one, is that they treat the quasi-classical worlds as non-interacting. Clearly, unitarity requires that this is just a convenient approximation.
Robin Hanson actually tries to get somewhere with using these interactions to get Born law-like behavior. Successfully? Well, I need to see the code he uses for his simulations, but it at least sounds promising. The basic idea is that the disturbance of one quasi-classical world upon another nearby is weighted _naturally_, _in the dynamics_ by the Born weights. Small worlds then get "destroyed" (nonsensical evolution, hence no observers that are human-like) by nearby larger worlds. But only "typical" worlds (i.e. ones having measurement records one would expect from Copenhagen) end up having non-negligible Born weights.