No, I wasn't arguing for that. What I assumed, as I said in an earlier post, was:
- There is a single random variable, [itex]\lambda[/itex], associated with the twin pair. This is chosen according to some probability distribution, [itex]P(\lambda)[/itex].
- When a particle reaches Alice, she has already picked a measurement setting [itex]\vec{a}[/itex], and her device is already in some state [itex]\alpha[/itex]. Then she will get result [itex]+1[/itex] according to some probability [itex]P_A(\vec{a}, \alpha, \lambda)[/itex] that depends on [itex]\vec{a}[/itex], [itex]\alpha[/itex] and [itex]\lambda[/itex].
- Similarly, when the other particle reaches Bob, he will get result [itex]+1[/itex] according to some probability [itex]P_B(\vec{b}, \beta, \lambda)[/itex] that depends on [itex]\vec{b}[/itex], [itex]\beta[/itex] and [itex]\lambda[/itex], where [itex]\vec{b}[/itex] is his detector's setting, and [itex]\beta[/itex] is other facts about his detector.
There is no assumption of determinism here. But there is no way to reproduce the perfect anti-correlations predicted by QM unless Alice's and Bob's results are deterministic functions of [itex]\lambda, \vec{a}[/itex] and [itex]\vec{b}[/itex], or unless there are nonlocal interactions (so that [itex]P_A[/itex] may depend on facts about Bob, or [itex]P_B[/itex] may depend on facts about Alice).