entropy1 said:
does that correspond with
I think you're making this more difficult than it needs to be. Have you read Bell's paper?
Here is Bell's line of reasoning:
We have a measurement of particle A and a measurement of particle B. These measurements take place at spacelike separated events.
At each measurement, we have settings, call them ##a## and ##b##.
If we do a large number of runs, we can construct a function ##E(a, b)## which gives the degree of correlation between the results as a function of the measurement settings.
Bell's locality condition is then that this function can be factorized: ##E(a, b) = F(a) G(b)##. Notice that each factor is a function of only one of the two measurement settings. He calls this condition "locality" because it appears to capture our intuitive notion that the results at one measurement should not depend on the settings at the other measurement, since they are spacelike separated. However, in the end it's just a mathematical condition; whether or not you think "locality" is a proper name for it is a matter of words, not physics or math.
Bell then shows that if the function ##E(a, b)## factorizes in this way, it must obey certain inequalities.
We know, however, that the function ##E(a, b)## which is predicted by quantum mechanics violates these inequalities.
Therefore, the function ##E(a, b)## which is predicted by quantum mechanics cannot factorize in the way described above, which means it violates Bell's locality condition. Therefore, quantum mechanics is "nonlocal" in this sense.