"No one can disprove an inequality like 2 < 3."
Exactly so. Leslie Lamport ("Buridan's Principle," 1984)addressed this problem of making a decision (or measurement) in a bounded length of time:
"A real Stern-Gerlach apparatus does not produce the discrete statistical
distribution of electron trajectories usually ascribed to it in simplified
descriptions. Instead, it produces a continuous distribution having two maxima,
but with a nonzero probability of finding an electron in any finite region
between them. Trying to decide if the electron is deflected up or down then
becomes just another instance of the problem of making a discrete decision
based upon a continuous input value, so nothing has been gained by
measuring the discrete spin value.
"Validity of Buridan's Principle implies the following:
"Buridan's Law of Measurement. If x < y < z, then any measurement performed in a bounded length of time that has a nonzero probability of yielding a value in a neighborhood of x and a nonzero probability of yielding a value in a neighborhood of z must also have a nonzero probability of yielding a value in a neighborhood of y.
"If this law is not valid, then one can find a counterexample to Buridan's Principle, with the discrete decision being: 'Is the value greater or less than y?' There does not seem to be a quantum-mechanical theory of measurement
from which one can derive Buridan's Law of Measurement."
Lamport goes on to describe the experimental challenge in terms of classical continuous functions:
"Buridan's Principle rests upon mathematical concepts of continuity and boundedness that are not physically observable. No real experiment, having finite precision, can demonstrate the presence or absence of continuity, which is defined in terms of limits. No experiment can demonstrate that an arbiter requires an unbounded length of time to reach a decision. An experiment in which the arbiter failed to decide within a week does not prove that it would not always decide within a year.
"To understand the meaning of Buridan's Principle as a scientific law,
consider the analogous problem with classical mechanics. Kepler's first law states that the orbit of a planet is an ellipse. This is not experimentally verifiable because any finite-precision measurement of the orbit is consistent with an infinite number of mathematical curves. In practice, what we can deduce from Kepler's law is that measurement of the orbit will, to a good approximation, be consistent with the predicted ellipse."
Joy Christian's experimental paraemters are classical, as were Bell's. His measure criteria, therefore, are predictive without being probabilistic. Any experimental model is finite in space and bounded in time. Quantum mechanical experiments assume that reality is finite in time (t = 1) and unbounded in space, therefore nonlocal. A local realistic model finite in space and unbounded in time is a classical measurement scheme that -- like Kepler's orbits -- makes a closed judgment to arbitrary accuracy of determined particle paths and momenta as t --> T, according to the specified topology in which the functions are complete, continuous and real.
Tom