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ajw1 said:Have you noticed they probably use a different model for their combined type I and type II experiments? They use something called a DLM (deterministic learning machine). This is not present in the model you base your conclusion on.
See"[URL Event-based computer simulation model of Aspect-type experiments
strictly satisfying Einstein’s locality conditions[/URL]
That is the reference I am working with. And yes, they refer to the DLM but it is not a part of their model as far as I can see except as general justification for their program. Their formula is arrived at as follows, quoting:
"... Therefore we use simplicity as a criterion to select a specific form. By trial and error, we found that T(n − 1) = T0F(| sin 2(n − 1)|) = T0| sin 2(n − 1)|d yields useful results. Here, T0 = max T() is the maximum time delay and defines the unit of time, used in the simulation and d is a free parameter of the model. In our numerical work, we set T0 = 1. As we demonstrate later, our model reproduces the quantum results of Table I under the hypothesis that the time tags tn,1 are distributed uniformly over the interval [0, | sin 2(n − 1)|d] with d = 2. Needless to say, we do not claim that our choice is the only one that reproduces the results of quantum theory for the EPRB experiments."
And again, since I am following their model which uses Type II PDC, I am sticking with that alone for my example. And I use that for the spreadsheet. However, the same problem does exist with Type I PDC so I don't think it is necessary to further document.
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