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| Tags: 1193, derivative, generalized, gravity, lie, quantum |
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From Osher Doctorow
The generalized Lie derivative for a pair of real variables (x, y) will be defined as: 1) L(x, y) = [x, y]* = xy + yx = 2xy where the notation [x, y]* is used to contrast xy + yx with the more common [x, y] = xy - yx used for ordinary Lie brackets with various other types of arguments x, y. Notice that in probability-statistics, xy is typically an indication of "statistical independence", defined by: 2) P(AB) = P(A)P(B) = xy, x = P(A), y = P(B) which is also equivalent to conditional probability P(B|A) = P(B) since P(B|A) = P(AB)/P(A) and if the latter equals P(B) then we get P(AB)/P(A) = P(B) or P(AB) = P(A)P(B), provided that P(A) is not 0. But "statistical independence" is the WRONG direction of (Probable) Causation/Influence, a fact which is easily remedied by examining: 3) L(x, x) = 2x^2, L(y, y) = 2y^2 This "Self-Independence" or "Self-Interaction" (depending on one's viewpoint) is not at all decreased by multiplication by a second variable, and so is arguably resembles x or y respectively in its role in (Probable) Influence/Causation. Thus, in the Riccati Differential Equation: 4) dy/dt = A(t) + B(t)y + C(t)y^2 we see that y and y^2 are respectively constant-interaction and self- interaction, or constant-independence and self-independence types of expressions: 5) L(y, 1) = 2y 6) L(y, y) = 2y^2 These resemble the roles of respectively momentum and energy with regard to velocity/speed in classical physics and the limiting cases of GR. Osher Doctorow |
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