The proof of: 1) If P(A) < 1/2 and P(A<-->B) = 1 + DEP(A, B), then P ' {(A --> B) | A)} > P(B) is direct from QG 347.3 by simply interchanging A ' and A in that theorem. Notice that P(A ' ) > 1/2 is equivalent to P(A) < 1/2 since P (A ' ) = 1 - P(A) > 1/2 iff P(A) < 1/2. Also recall that we have P (A<-->B) = P(A ' <--> B ' ), proven a few posts back. Notice that (1) says that under the conditions of P(A) < 1/2 ("low probability events) and with the interpretation of P(A<-->B) as 1 + DEP (A, B), then the Probable Causation (P ' type) of B by A with A "given" or fixed is higher than P(B), which intuitively corresponds to positive Dependence since Statistical Independence is equivalent to P (B|A) = P(B) when P(A) is not 0. The latater equation P(B | A) = P(B) when written out is P(AB)/P(A) = P(B), or P(AB) = P(A)P(B). In terms of the Statistical Dependence DEP(A, B) = P(AB) - P(A)P(B), the latter statement says DEP(A, B) = 0, while DEP(A, B) > 0 is equivalent to P (AB) - P(A)P(B) > 0 which is equivalent to P(AB)/P(A) > P(B) or P(AB) | A) > P(B). The implications appear to be considerable. Dependence of (random) variables cannot be understood in general without Probable Causation/ Influence (PI) and its linkage to mainstream Statistical (Quadrant) Dependence. Foundations of Quantum Probability/Statistics that do not account for this, whether as special cases or limiting cases, become questionable. Information Theory, which makes extensive uses of Conditional Information, Mutual Information, etc., is also restricted by the same requirements, and again Quantum Information is affected. Osher Doctorow Other posts:
• Quantum Gravity 347.5: P ' {(A --> B | A) } = P(B)[1 - P(A)]/P(A) is
Equivalent to y = y(0) t exp(-t)
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