stevendaryl said:
The point was that local doesn't mean "no FTL signals".
In some sense the whole issue of QM and "FTL" is a bit of a red herring - an interesting shade of red to be sure. And maybe the discussion should also take into account causality.
Clearly there are situations in which something I do 'here' affects something over 'there'. If I hit a golf ball here it will, some time later, cause a splash there - at least if I'm hitting it anyway. But in relation to QM the issue is whether a measurement I do here affects 'reality' there. I don't think QM, strictly speaking, forces us to adopt that position.
But for me the local/non-local thing isn't what's most fascinating. I think the Bell inequalities show us that classical theories are in big trouble before we even consider measurement events that are spacelike separated. Of course it's important to have the spacelike bit if we want to rule out
local hidden variable theories.
If we're not worried about the spacelike bit then we could, in principle, construct a hidden variable theory that might explain the violation of the Bell inequalities that would be local - but I think any such theory would be artificial and somewhat ad-hoc. It would be hard, I think, to construct a general hidden variable theory to account for all of the possible entanglement experiment variants we might conceive - and such a theory would probably be as far removed from what we might consider 'classical' physics to be as QM is (on the surface at least).
I'm not sure I would consider the Bohm version to be the kind of theory I'm talking about here. That seems to me to be a kind of sleight of hand - it essentially takes QM as its starting point anyway and just redefines things a bit to give us this unexplained complex guiding potential - so it's a theory that's explicitly constructed to be the same as QM that ultimately doesn't explain anything.
So even without all of the endless FTL/non-local tongue-twisting I think entanglement implies that our description of the world must be very different from what is traditionally understood as classical physics.