Or, through a simple, deterministic, arguably classical, mechanism using only speed-of-light interactions as described and linked to above, but here again for convenience:
https://docs.google.com/open?id=0BxBGJRkQXyjweXR2R3ExTlEyNm8
Per Occam's Razor, would you turn first to speed-of-light interactions from E to A and E to B that operate for an interval of time, or an instantaneous interaction between A and B? The former, of course. Unless you have a grant application pending for yet another EPR experiment? I've most certainly shown that the former can achieve the same results as QT and I have (you can too) tweaked the simulation to match any EPR experiment performed thus far.
The simulation I provide in the paper can even be implemented in circuitry with space-like separation between A and B. It will certainly result in CHSH > 2, over a broad range of random walk step sizes of the signal from E to A and E to B as well as over a broad range of coincidence windows.
In other words, I believe the game has been changed, pending experimental confirmation that nature actually works this way. But, Occam clearly suggests what experiment to do next (hint: not another traditional CHSH).
Michael B Devine