Wow, I haven't checked back on this thread in a little while. I wasn't expecting so much activity.
Demystifier said:
No!
Poisson equation is local, but acceleration of ONE particle CANNOT be calculated by knowing ONLY the solution of the of the Poisson equation and position of that particle. Instead, you must also know the positions of all other particles.
I believe I disagree with you on interpretation here.
Just because you need to know the positions of all other particles to calculate the gravitational field does not make Newtonian gravity non-local in my eyes.
The dynamics still arise from the Poisson eq, which is a local law. However, the Poisson equation's field propagates infinity fast, so we need to know all of the positions of each particle to calculate the dynamics accurately.
So to me, this is "non-local" in the sense that it is local, but that the field propagates infinitely fast.
And IMO, this is great because when we go from Newtonian Gravity to GR, the propagation speed changes from infinity to c. Clearly then, the gravitational field is local by just about anyone's definition.
Similarly, in dBB, we have that the dynamics of the theory (at least if we talk about the theory involving a wave function in configuration space), are local but propagate infinitely fast. Of course it is also strange that the wave function is defined not in space, but in configuration space.
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Edit: I should mention that below I'm talking about vanilla relativistic QM, and that I haven't studied this myself, so my understanding is via small discussions with my roommate. That is to say, I have no reason to believe I haven't said something wrong.
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If we change to the Klein-Gordon equation, we still have a local law with infinitely fast propagation, but if we use the Dirac equation(s), we have particles & anti-particles that travel no faster than speed c. We get multiple local disturbances that propagate at finite speed and conspire together to create a law that looks non-local.
So the way it looks to me is: in Schroedinger-dBB, we have non-local dynamics that arise from a local law with infinitely fast propagation. When we move to the relativistic limit with the Dirac equation, this propagation becomes only finitely fast.
If what I have said is accurate (and I have my doubts), then I see no problem with calling dBB local (but with infinite propagation speed)