Gordon,
"I'd be pleased if you'd check the wording of your second paragraph and post it here (unchanged if you wish) for critique/discussion. ...As it's written, it makes no sense to me."
(Ref PJ Jul. 7, 2014 @ 17:33: "I hope you'll give the short summary a very careful read and rigorous criticism." Classical reproduction of quantum correlations. ) Delighted;
"Bohm's Gedanken experiment described a pair of particles, one spin 'up', one 'down'. On reaching distant separated Stern-Gerlach magnets if 'A' deflects up, 'B' goes down, strangely not evenly distributed but giving two 'bunches' on the screens. If magnet A is rotated; the particle deflects down. The particle at B then MUST go up. Therein is the problem. If magnet A is reversed at the last moment, how can B know without "spooky action at a distance"?
I confess it is overly 'condensed'. A diagram of Bohm's thought experiment would help, simply a central source splitting and sending 'entangled' particles in opposite directions to (Bob and Alice's) 'rotatable angle' magnets which deflect them. At identical angles we find opposite deflection (or 'particle spin'). At 'opposite' angles, we find identical deflection (spin) direction. But that gives the big issue; Reversing magnet A at the last moment DICTATES particle B's deflection/ spin state! !
How can 'B' instantly know A's setting, and which 'way up' it must be when its a light year away?! That's QM's 'spooky' non-locality. (The cause of the non-linear 'bunched' distribution of deflections is a related but separate issue).
I then show how BOTH issues are logically resolved by using a different 'starting assumption' to Bell. He assumed multiple 'random' (but each pair 'opposite') spin axes for the particles. The DFM schema is based on optics Huygens construction and the NLS equation; Effectively 'dipoles' propagating on the spin axis so describing twin helical paths (a single helix, torus or sphere propagating axially works fine for 'polarity'). The interaction with the detectors EM field electrons is then dictated by the detector setting, so each detector can 'flip' the spin. The key is that N/S spin POLES are entirely random.
100% of Aspects (assumed 'anomalous') data is then predicted (he had to discarded almost all of it). Statistically based analysis of multiple events can't distinguish pairs and uses the wrong assumption. In the DFM schema A can change setting and B is free to find either UP or DOWN entirely at random.
That does take a little getting your head around at first. Did you understand how the intermediate cos2 distribution naturally emerged from the angular momentum exchange ('measurement')?
If anyone else is struggling with it do just ask. Grasping the model before 2020 puts you well ahead of the game! Conceptually it may help to think of the distribution of spin speed with changing latitude on the surface of Earth.
Best wishes
Peter