By Robert B Ash; Catherine Doléans-Dade
ISBN-10: 0120652021
ISBN-13: 9780120652020
Read Online or Download Probability and measure theory PDF
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Extra resources for Probability and measure theory
Example text
3 Definition of the Integral. 7. We define = L~=l xJA, as long as +oo and -oo do not both appear in the sum; if they do, we say that the integral does not exist. Strictly speaking, it must be verified that if h has a different representation, say LJ=I yjls1 , then ~ r s LX;jt(A;) = LYjtt(B;). ) The proof is based on the observation that r h= L L ZijlA,nB 1, i=l j=! where Zij = x; = Yj· LZijtt(A; i,j Thus n Bj) = 2:x; Ltt(A; n Bj) by a symmetrical argument. If h is nonnegative Borel measurable, define simple, This agrees with the previous definition if h is simple.
4) The set function JL is countably additive on 9Q(in). ~,(llt) is finite. If a E ~n. 8(b); if a E "in - ~n, the same result holds by (3). 3. ~,("in) = oo. Then F, restricted to Ck = {x: -k PRooF. First assume that F ( oo) - F ( -oo) < oo, so that JL is finite. Let A 1 ,A2, ... 9{i("i) decreasing to 0. If (a, b] is one of the intervals of An, then by right continuity ofF, JL(a', b] = F(b)- F(a') --+ F(b)- F(a) = tt(a, b] as a'--+ a from above. 90("1) whose closures Bn (in "i) are included in An, with tt(Bn) approximating tt(An ). If£ > 0 is given, the finiteness of JL allows us to choose the Bn so that tt(An) - tt(Bn) < e2-n. Now n~ 1 Bn = 0, and it follows that n~=t Bk = 0 for sufficiently large n.
Probability and measure theory by Robert B Ash; Catherine Doléans-Dade
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