
Originally Posted by
MorpheusSandman
You say the "quantum stuff is real," but both CI and CH define the wavefunction as non-real. It's only MW that assumes it's real.
Whether the wavefunction is real or not is not the question. That is the mathematics that represents it. Personally, I don't think it is real, but it doesn't matter. The quantum stuff, things like electrons and photons, are real in the common sense definition of real. Some of the properties about them are not certain. That is what makes these properties unreal, but the underlying stuff that could have these properties is "real".

Originally Posted by
MorpheusSandman
Decoherence + realism requires MW. Decoherence can't work in CI because of CI's collapse (the collapse and decoherence are mutually exclusive). If you assume decoherence but non-realism you get CH, apparently.
I'll stick with CH to avoid using the wave function in these discussions.
I claim that if realism requires determinism, not even MW can provide this since the facts of the matter are the quantum stuff is not deterministic. MW hopes it will one day get around the problem that the facts present, but it has yet to produce an interpretation that is complete enough to generate even one wave function.
Perhaps it is important to make explicit just what it means to not be able to produce the Born probabilities. What that means is that MW cannot produce the coefficients for even the simplest wave function.
The only interpretation I am aware of that is deterministic and complete enough to generate a wave function is Bohm's interpretation which is superdeterministic (we are in the Matrix without any Zion-like resistance movement) and deliberately non-local.

Originally Posted by
MorpheusSandman
What in the world makes you think MW has to have only two worlds? Keep in mind that in the double-slit experiment with one particle, through different trials you have the particle going through either, both, or neither slit. Since MW takes the wavefunction as real, this would itself imply 4 distinct "worlds" (possibilities) within the wavefunction (within that test, at least). Besides, you have to keep in mind General Relativity in terms of measurement; there is no universal "now," merely different perspectives in space. So no two measurements of the same particle could be simultaneous since there is no simultaneous time. One observation has to happen "first" (Implying one is first shows the limitations of the language keeping in mind the perspective aspect of GR), and once it happens decoherence happens locally; so the other observer is no longer observing the same wavefunction of the same particle. The apparent affect happens as a result of decoherence.
Because the two particles are entangled, once the data from the two observers is matched a correlation needs to be observed to account for the quantum facts. How is that accomplished in MW?
I've tried to find how this might be answered and so far have only found three kinds of answers.
1) Claim that the experimental data showing non-locality is incorrect. This would avoid the problem entirely for all interpretations. I understand that the tests are still being refined to eliminate any loopholes, so there is a slight possibility this might work. Of the three, this is the only valid argument.
2) Claim that it can't happen in MW, but not explain why. For example, here is Lev Vaidman's comment (http://plato.stanford.edu/entries/qm-manyworlds/)
The most celebrated example of nonlocality was given by Bell 1964 in the context of the Einstein-Podolsky-Rosen argument. However, in the framework of the MWI, Bell's argument cannot get off the ground because it requires a predetermined single outcome of a quantum experiment.
However, after the data was collected, not only did it "get off the ground", but now MW has to get off its butt and account for it.
3) Claim that there is some third measurement that patches all this together. Here is Frank Tipler's comment (http://arxiv.org/pdf/quant-ph/0003146v1.pdf):
Furthermore, this ignored third measurement is actually of crucial importance: it is performed after information about the orientation of the second device has been carried back to the first device (at a speed less than light!). The orientation is coded with correlations of the spins of both electrons, and these correlations (and the linearity of all operators) will force the third measurement to respect the original split.
How does this happen in MW? That is the problem. It is not enough to just state that it all works out in the end.