Bell's theorem has nothing whatsoever to do with any of that. Bell's own view was that his theorem indicated a potentially disturbing incompatibility between quantum physics and relativistic causality, and not that it implied space was an "aether" or anything like that. Even there, that Bell expressed this view does not mean anyone reading it is obligated to agree with it.
One does not need much more to end up with an ether.
All one needs is a complete causal theory - causal in the sense of Reichenbachs principle of common cause, and of the non-existence of causal loops.
Then, Reichenbach's principle of common cause gives us that for the observable correlation A = -B there has to be a causal explanation, which is or a causal influence A->B, or B->A, or some common cause C->A, C->B. Then, Bell's theorem shows that the common cause explanation leads to Bell's inequalities, thus, can be excluded experimentally. It remains or A->B, or B->A. If QM is universally true, this holds for arbitrary pairs of events, except for may be some degenerated cases of measure 0.
Above A->B and B->A cannot be true at the same time, this would be a causal loop. Thus, a causal theory has to tell us what is true - A->B or B->A, for all pairs of events, else it would not be complete. Then, if there are no causal loops, the relation A->B defines an order. The future of A, F(A) is what can be influenced causally by A, the past P(A) what can causally influence A, and the present is the intersection of their closures, and given that for every event B there is arbitrary close some event B' so that Bell's inequality is violated for (A,B'), B' is or in the past or the future, thus, B or in the closure of the future or of the past, thus, itself of past, present or future.
Thus, a complete causal theory contains a preferred time-like foliation.
The next step, given a preferred foliation, is the ADM decomposition of the metric into a scalar field, a three-vector field, and a three-metric. One can, then, try to interpret them as density, velocity, and stress tensor of the ether.