DrChinese said:
Thanks, that's helpful, because there are SOOOOOOOO many errors packed into your 2 short paragraphs. If you went faster, I'd no doubt miss some of them.
2 entangled particles can be measured separately in any 2 directions, let's call them a and b. QM says that there is a statistical relationship between the expected outcomes. That is the end of the story for QM.
All right.
But ANY realistic theory postulates that there are simultaneous values for any other set of directions, c/d/e... whatever.
Bohm's theory doesn't postulate that. So it isn't a realistic theory by your definition of that term? This just goes to show that your definition of that term is pointless/misleading/vague/sloppy.
The idea is that those values are real and definite INDEPENDENT of the ACT of OBSERVATION. So let's focus on c, that is enough to get the idea across. Prepare an equation which shows the relationship between a, b and c and you will immediately run into the Bell Inequality.
You have to be more careful. Here's an equation that involves all three. Say, for electrons whose spin is completely random (coming out of an oven or something, so the spin part of the density matrix is proportional to the identity matrix)
P(a) + P(b) + P(c) = 3/2
where P(a) = the probability for the electron to be measured as spin-up along the a-direction if that measurement is made. This is a perfectly well defined and valid equation even in the context of orthodox QM. My point is just that you can't point to an equation that involves these 3 variables and infer *on that basis alone* that there is something unphysical or untoward going on, such as a presumption that 3 incompatible measurements all happen at once. There is no such presumption in the above equation, and also none in Bell's equations that you always point to.
That said, it is true that those equations you point to in Bell's paper do not pertain to orthodox QM. They contain, after all, functions like A(a,lambda) which denote the outcome that would obtain if a measurement is made along direction "a" when the particles are in state lambda. (Somewhat more precisely, this denotes not the actual outcome of any actual experiment, but the prediction of the deterministic theory in question here for such an experiment.) This is what leaves me so confused about your obsession with "c". In Bell's paper, we have
P(a,b)
and
P(a,c)
as the correlations when the pair (a,b) is measured and when the pair (a,c) is measured. If Bell started talking about P(a,b,c) -- the correlation when all three quantities are measured at once -- then I guess you'd have him, since it's not possible to measure all 3 at once. But he doesn't, so what the heck is your problem? What are you objecting to? Surely it's perfectly sensible for a theory to make some kind of prediction for P(a,b). And surely it's sensible for a theory to make some kind of prediction for P(a,c). And surely it's sensible to take those two numbers and subtract them... just like, in OQM in my example above, there is a well-defined quantity P(a) = 1/2 and another well defined quantity P(b) = 1/2, and another well-defined quantity P(c) = 1/2, and once you have those, there's nothing the slightest bit illegal about adding those up to find 3/2. Of course, if you are mentally challenged and you think that this means "when you do a magic experiment that measures all 3 quantities at once, your experiment will have outcome 3/2" then, sure, that's a problem. But it's your problem, not the problem of the theory. And likewise with Bell's consideration of P(a,b) - P(a,c).
And to repeat what I said before, why in the world do you only start fussing about "c", when already Bell has defined A(a,lambda) in a way that is completely at odds with orthodox QM? I mean, once you allow *that*, then there is no valid way to object to anything that happens later (as I tried to explain in the last paragraph). In OQM, there is no such function as A(a,lambda), right? First off, OQM isn't deterministic, so the idea of there being a *function* which specifies *the outcome* for a given setting, is clearly at odds with OQM. Furthermore, in OQM, specifying "a" and the state of the pair (lambda = the 2 particle wf for OQM) is *not* enough information even to predict the *probabilities* of possible outcomes. The theory is nonlocal in the sense that you must specify also some information pertaining to bob's experiment in order to define (even) the probabilities for Alice's. So in at least these two ways, the function
A(a,lambda)
is at odds with OQM. So if you're going to object to something in Bell's derivation, it should be *that*.
But of course, as I've also explained to you a million times, that objection isn't going to work, because Bell has a *reason* for making this un-orthodox assumption of functions like A(a,lambda). He describes it quite clearly in the opening paragraph of his paper when he says:
"The paradox of [EPR] was advanced as an argument that [QM] could not be a complete theory but should be supplemented by additional variables. These additional variables were to restore to the theory causality and locality." He doesn't rehearse the argument here, but the point is that he is citing EPR as proving that the "hidden variables" -- in particular, some variables which locally determine the outcomes once the state of the pair (lambda) and the local setting (a) are specified, i.e., just exactly the functions A(a,lambda) he uses later in the paper -- must exist *in order to restore locality*, which means: in order to replace the *nonlocal* theory OQM with something that is local. In short, he cites EPR as showing that Locality requires exactly the kind of un-orthodox HV's he uses later in the paper. Got it?
Of course, the conclusion of the paper is that this strategy fails. You can't get the empirically correct predictions with those local deterministic hidden variables... which means that, since those variables were required in the first place as the only possible way of saving locality, locality cannot be saved... which Bell says quite clearly in his opening paragraph: "It is the requirement of locality, or more precisely that the restult of a measurement on one system be unaffected by operations on a distant system with which it has interacted in the past, that creates the essential difficulty." He also mentions Bohm's theory as a counterexample to a bunch of earlier (bogus) impossibility proofs, and notes that Bohm's theory "has indeed a grossly nonlocal structure." He then restates what the main conclusion of his paper will be: "This [the nonlocal structure] is characteristic, according to the result to be proved here, of any such theory which reproduces exactly the quantum mechanical predictions."
So to summarize:
1. Your objection about "c" makes no sense
2. If you are going to object to something, you should object earlier -- to Bell's equation (1)
3. But don't bother, because the answer to that objection is the EPR argument as discussed quite clearly by Bell in this paper and many others.