| |
Re: Measurement Pb in Quantum Theory |
 | | Interestingly the wavefunction of the universe is not normalisable (a least not for any models i've since in the literature), so we don't get probablities here. |
 | | This is >because the number of distinct orthogonal wavefunctions over >which the density matrix of any thermal system can be expanded is >of the order of exp(S/k) where S is the entropy of the system and k >is Boltzmann's constant. |
 | | Yes, you've got the maths right here, but you when you change the resolution of the splititing you also increase the number of different worlds the observer is in, overall the relavitive states at the courser level is an approximation of the one at the fine level, and probablities should remain about the same. |
| www.lns.cornell.edu /spr/2000-07/msg0026443.html (1448 words) |