Demystifier said:
But Bell has shown that superluminal influences are not an exclusive property of BM per se, but of ANY theory (compatible with QM) claiming that reality (i.e., objective physical properties existing even without measurements) exists. My impression is that most physicists who complain about superluminal BM influences are not aware of this general Bell's result.
Well one can still argue that we deal with 'non-classical correlations' without any 'action-at-distance' involved. How can Nature conspire, in non-classical ways, to produce the appearance of action-at-distance is another thing but I wouldn't take lightly the 'conspirational hypothesis'; superdeterminism for example is fully compatible with all experiments conducted so far (it may lack 'le bon sens', to quote Duhem, but counterfactual definiteness is by no means untouchable).
And a few questions regarding Bohmian Mechanics (as I see you know it very well):
1. How it is explained within BM the fact that electrons do not fall into the nucleus? (as far as I know Vigier proposed the hypothesis that a radiation of very long wavelength is indeed emitted by the electrons but we aren't yet capable to measure it).
2. If the guiding wave affect the particle shouldn't the particle affect the wave as well? If the answer is yes how is this happening?
3. Why is Lorentz invariance so important? As far as I know there are indeed reformulations of Special Relativity - involving some changes at the level of the basic postulates but indistinguishable at the experimental level from the classical solution (based on the usual Lorentz transformations) - where a preferred frame of reference is accepted (thus fully compatible with Bohmian Mechanics). But my point is that although (local) Lorentz invariance is part of the accepted methodologies in Physics (I accept that it has a provisional edge over the alternatives) it is by no means required with necessity by the observed facts (anyway the Brans-Dicke theory etc are still with us). I wouldn't be surprised if a final (successful, the 'winner') TOE is not Lorentz invariant...
4. Why the density of probability P tends towards |PSI|^2, isn't this an ad-hoc hypothesis? (some accuse the ad-hoc nature of Bohm's explanation, namely that the value of P is pushed towards |PSI|^2 by aleatory interactions and the quantum dynamics, more or less like in the classical statistical mechanics).
5. Do you believe that a non-trivial change at the level of the basic postulates of QM could make a difference between the existing interpretations of QM, by pointing towards a clear 'winner' (possible an unconceived yet alternative)?
6. Are there other promising (non-local) hidden variables programs?
7. The spin?...but of course there is no real problem to consider it a phenomenological property