Joy Christian wrote:FrediFizzx wrote:
Yeah, the Bell fans are finished and don't even know it. They think because they have moved the goalposts to Gill's "theorem" that they are not finished. But it is just junk physics like Bell's junk physics theory. It has nothing to do with comparing local models to quantum mechanics since QM can't predict individual event by event outcomes either.
The traditional proof of Bell's theorem depends on the following assumption (without the question mark). Note that the indices j and k and the settings b and b' are not the same:
Although I accept the above equality in
my paper, I am curious whether it even holds for the real experiments where they have observed only 256 events. It is supposed to hold for large values of p and q. But how large would they have to be? Any way to check that? Perhaps this is a question for a statistician.
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Joy, perhaps I'm misreading it.
BUT it seems to me that there is a mistake in the above assumption; the one that you associate with the traditional proof of Bell's theorem.
Without any reference to QM, one finds, via the ordinary definition of an average or expectation, under EPR-Bohm (the experiment studied by Bell in 1964):
(1) The LHS = E(a,b) = -cos(a,b) ideally. (2) The RHS = E(a.b') = -cos(a,b') ideally.
THUS: The "questioned-equality" can be replaced by ≠ if b ≠ b'. And by = if b = b'.
PS: Please, can you show me where it occurs in Bell (1964) or in any other Bellian work?
And which equation are you referring to when you say you accept it in your paper?
Thanks; Gordon
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