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Ariel Cheng's avatar

> For that kind of problem we’d need to defer to law, history and analytic philosophy - all which have styles of thinking that have nothing to do with experiments.

What about thought experiments?

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Han's avatar

Dear Physics Enjoyer

Thank you. Allow me please to make the following comment.

Here, I present a short description of the statistical analysis of Aspect's experiment.

The x is angle(a,b) in [0,2π).

The, a, is Alice's instrument parameter vector. The, b, is Bob's instrument parameter vector.

The angle is measured in the plane orthogonal to the A-S-B axis. This “orthogonal to the A-S-B in the plane variation of x" is sufficient variation for understanding the statistics of the experiment. It is also physically valid.

Note furthermore that the experiment is embedded in classical probability theory. E.g. the law of large numbers to estimate the probability space behind the Bell correlation formula.

Aspect then requires:

1. cos(x)= P(x,=) - P(x,≠)

1a. P(x,=)=N(x,=)/N

1b. P(x,≠)=N(x,≠)/N

1c. N(x,=)=N(x,+,+)+N(x,-,-)

1d. N(x,≠)=N(x,+,-)+N(x,-,+)

1e. N=N(x,=)+N(x,≠)

2. cos(x)=1-2sin²(x/2), x in [0,2π)

3. P(x,=)+P(x,≠)=1

4. P(x,≠)=sin²(x/2), x in [0,2π)

The left-hand in 4. is a data probability (estimate) determined by nature. The right-hand isn't a probability function. It isn't monotone non-descending for x in [0,2π).

5. For x in [0,2π), the alleged associated probability density is f(x)=(1/2)sin(x).

5a. This alleged probability density is derived from 4. via f(x)=dF(x)/dx. But observe, f(x)=(1/2)sin(x), x in [0,2π), isn't a probability density. It isn't positive definite for x in [0,2π).

5b. This f(x) results in negative probabilities and other violations of Kolmogorov axioms.

5c. There are absolutely no classical probability model assumptions necessary for the presented statistical analysis in order to describe the entanglement correlation.

6. Obviously, x is a part of the random variable X describing the event “x,≠” in the measurement.

7. The x is entirely free to have any value in [0,2π), in order to maintain Einstein locality.

If an experiment violates Kolmogorov axioms, it's invalid. In fact, potential Einstein positive data is excluded from observation by requiring, e.g., a not positive definite probability density for that data. That's clearly a nonsensical requirement.

Aspect's experiment is statistically flawed.

Hence, also within science, the scientific method can fail.

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