Quantum Gravity 191.3: Proof of Theorem



 Science > Physics > Quantum Gravity 191.3: Proof of Theorem

LINK TO THIS PAGE  


rating :  0   |  0


  Page 1 of 1
Topic: Science > Physics
User: "OsherD"
Date: 20 Oct 2007 08:48:54 AM
Object: Quantum Gravity 191.3: Proof of Theorem

From Osher Doctorow

The Theorem in 191.0 is proven as follows, with the slight
modifications of the Theorem indicated below in the case of (1) of
191.0.
(1). If B is a subset of A with probability 1 (w.p.1), then AB = B
(w.p.1) so P(AB) = P(B) so P(A-->B) = P(A). Therefore P(A-->B) = P
' (A-->B). But P ' (A-->B) = 1 + P(B) - P(A) with P(B) < = P(A) = 1
iff P(B) = P(A), and since B is a subset of A (w.p.1), since means
that B is a maximal such subset (w.p.1).
If A is a subset of B (w.p.1). then P(AB) = P(A) so P(A-->B) = 1. P
' (A-->B) = 1 + P(B) - P(A) with P(B) < = P(A), but since A is a
subset of B (w.p.1), we must have P(A) < = P(B) by monotonicity of
probability so P(A) = P(B), so P ' (A-->B) = 1.
(2). If A is not a subset of B (w.p.1) and B is not a subset of A
(w.p.1) but they are disjoint, then P(A-->B) = 1 + P(AB) - P(A) = 1 -
P(A) = 1 iff P(A) = 0. But P ' (A-->B) = 1 + P(B) - P(A) = 1 iff P(A)
= P(B), and the latter may or may not hold for disjoint sets depending
on the particular sets. So P(A-->B) is optimal (1) when P(A) = 0,
but there is no general optimization of P ' (A-->B).
(3) In the case of (2) above except that A and B are not disjoint (w.p.
1), this means that P(AB) > 0. But P(A-->B) = 1 + P(AB) - P(A) = 1
iff P(AB) = P(A) iff A is a subset of B (w.p.1) which is false, so
P(A-->B) cannot be optimized (at 1). P ' (A-->B) is as in (2) above.
Osher Doctorow
.


  Page 1 of 1


Related Articles
Quantum Gravity 180.6: The Modified Unit Diagonal Theorem for PI Matrix
Quantum Gravity 169.2: Fermat's Last Theorem Equation x^n + y^n = z^n In PI Phase
Quantum Gravity 180.8: Random Variable Diagonal Matrix Theorem
Quantum Gravity 231.0: The g-theorem in Combinatorics Via ProbableCausation/Influence
Re: Quantum Physics bifurcation of Plant versus Animal kingdoms in
Learning to be a Quantum Mechanic
Elementary Heat Quantum
Simple quantum mechanics question
THE QUANTUM BRAHMAN
Re: Quantum computer using using artificial atoms.
macroscopic quantum wavefunctions
Quantum Complex Stochastics
Quantum Gravity 30: QCD and Gravitation
Quantum Gravity Via Expansion-Contraction 2.3: Projectile Range cs Resistance and Crosswind Via W
Quantum Gravity Via Expansion-Contraction 6.0: Riccati 2 Version Using Special Relativity Beta Squared
 

NEWER

pg.1612     pg.1232     pg.940     pg.716     pg.544     pg.412     pg.311     pg.234     pg.175     pg.130     pg.96     pg.70     pg.50     pg.35     pg.24     pg.16     pg.10     pg.6     pg.3     pg.1

OLDER