FrediFizzx wrote:As expected; complete denial. LOL!
Perhaps you should have read section II. "Bell Inequalities for Continuous Variable Systems" before you made your comments. But that is OK; perhaps it is too much physics for you.
Yes, that section should be interesting. There are generalized Bell inequalities for variables taking any number of values, even continuously many ones. In my work with Stefan Zohren on the CGLMP (Collins, Gisin, Linden, Massar, Popescu) inequality, see for instance
http://arxiv.org/abs/1003.0616, Europhysics Letters 90 (2010) 10002, S. Zohren, P. Reska, R. D. Gill, W. Westra, "A tight Tsirelson inequality for infinitely many outcomes", we showed that in the limit of continuously many outcomes for this most simple generalization of CHSH to the case of more than two outcomes, we get a continuous variable Bell type inequality which actually coincides with the corresponding generalized Tsirelson inequality: i.e., quantum mechanics and local realism are subject to exactly the same bound. In other words: when we go to continuous variables, Bell and Tsirelson inequalities coincide: local realism can do everything that QM can do. It is amusing that in this limit we are back with the original EPR example of measuring position and momentum Q or P on two particles, except that we measure Q or P on one of the particles, Q + P or Q - P on the other. Moreover it turns out that in order to achieve the bound, one should not use a maximally entangled pair: one should *not* use the singlet state!
In the meantime, equally off topic, did you understand now the meaning of the variable eta, Fred? The physical significance of eta was that actually in my theorem we are comparing two functions: the cumulative probability distribution function of S - 2, ie the function
"eta maps to Prob(S - 2 <= eta)", and the function "eta maps to max(0, 1 - 8 exp( - N (eta/16)^2 ))", which is another cumulative probability distribution function. In fact it is a probability distribution of well known type related to the Rayleigh distribution. The right tail of the distribution is of Gaussian type, decreasing very fast to zero; all moments are finite; it is a very nice, very "tight" probability distribution in fact. To say it in other words, the probability distribution of sqrt(N) ( S - 2) is stochastically smaller than a fixed generalized Rayleigh distribution. S can be larger than 2 but with large N, large deviations rapidly become very, very exceptional. Large deviations scale at the standard one over square root of N rate.
Back to the work of the Indian gentlemen Priyanka Chowdhury, A. S. Majumdar, G. S. Agarwal: obviously, an elementary true mathematical theorem cannot have a counter-example. Bell's theorem is truly a tautology, and it is a simple tautology at that. So if they claim to have found a classical physical system which violates Bell's theorem then, translated into mathematics they have found a mathematical system which violates Bell's theorem hence also, logically, does not satisfy the conditions of Bell's theorem. So instead of chortling with joy that Bell has been proven wrong, one should take this as an opportunity to more fully grasp what Bell is about. The title of the paper "Nonlocal continuous variable correlations and violation of Bell's inequality for light beams with topological singularities" with first sentence of the abstract "We consider optical beams with topological singularities which possess Schmidt decomposition and show that such classical beams share many features of two mode entanglement in quantum optics ... " show that the authors don't understand Bell's theorem but have come up with a classical physical system which reproduces some features of quantum mechanics but not, however, in the context of Bell's theorem, ie not in a context in which the corresponding experiment would tell us anything about locality and realism. The corresponding experiment would be an experiment with one of the famous loopholes: the loophole allowing a local realistic explanation!
So it is a very nice pedagogical exercise for people like Fred and Harry to think carefully about a loophole-free Bell type experiment, and think carefully about the experiment belonging to this paper, and to identify the "relaxation" which allows violation of a Bell type inequality by a local realistic system. I would prefer that you, the students, do this exercise yourself in your own time, before I, the teacher, reveal the solution.
Actually I didn't read the paper yet because I am concentrating on some other work at the moment:
http://bengeen.wordpress.com/,
http://arxiv.org/abs/1407.2731.