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Algebras and Maps

Dalam dokumen Ergodic Theory (Halaman 164-170)

Conditional Measures and Algebras

5.4 Algebras and Maps

Moreover,

[x]A =φ1(φ(x))

for x /∈ N, and μAx = νφ(x) for some measurable map y νy defined on a φμ-conull subset of Y. In fact we can take Y = M(X), φ(x) = μAx , andνy =y.

This will be proved later; the conclusion described in Corollary 5.22 is depicted in Fig.5.3.

Fig. 5.3 EachyY determines an atomφ1(y) and its conditional measureνy

Lemma 5.23.If X is a compact metric space, and f L(X), then the map

M(X)ν −→

fdν

is Borel measurable. In particular, for a Borel subset X of X, we have that M(X)is a Borel subset of M(X). Moreover, if φ:X →Y is a Borel measurable map between Borel subsets of compact metric spaces, then the induced mapφ:M(X)→M(Y)is Borel measurable.

Proof. Starting with continuous functions, we know that

fdν depends continuously onν (by definition of the weak*-topology on M(X)). Arguing just as we did on p.139, this can be extended to show that

fdν depends measurably onν for all indicator functions of open sets, and thence to show that it does so for indicator functions of Borel measurable sets, and finally for anyf ∈L. By definition and the argument above, it follows that

M(X) ={μ∈M(X)(XX) = 0}

5.4 Algebras and Maps 147

is Borel measurable. Now letφ:X →Y be measurable and fixr∈R,ε >0 andf ∈C(Y). Then

Of,r,ε =

μ∈M(Y)|fdμ−r< ε is an open set inM(Y), and clearly

φ1Of,r,ε=

ν∈M(X)|f◦φdν−r< ε

is measurable in M(X). Since any open set in M(Y) can be written as a countable union of finite intersections of sets of the formOf,r,εwithf chosen from a dense countable subset ofC(X),r∈Qandε∈Q, the lemma follows.

Proof of Corollary 5.22. Let A = σ({A1, A2, . . .}) be countably- generated. TakingY =M(X) (with the weak*-topology, so thatY is a com- pact metric space) andφ(x) =μAx we can set νy =y and henceνφ(x)=μAx follows at once. LetX be aμ-conull set on which all the statements in The- orem5.14hold. We claim first that (perhaps after enlarging the complement ofX by null sets countably often),A =φ1BY. By Theorem5.14(2),

χAi(x) =μAx(Ai) (5.12) for almost everyx, and we may assume that this holds for allx∈X. Since | ν(Ai) = 1} ∈BY, (5.12) shows that Ai∩X φ1BY and therefore A|X ⊆φ1BY.

For the reverse directionφ1BY ⊆A|X, it is sufficient to check this on sets of the formOf,r,εsince these generate the weak*-topology in a countable manner, and by Theorem5.14(1) the set

φ1 {ν| |

fdν−r|< ε}

={x| |

fdμAx −r|< ε}

isA-measurable for anyf ∈C(X),r∈Randε >0. HenceA|X =φ1B. Sinceφ:X →Y satisfies A|X =φ1BY, and the Borelσ-algebraBY

ofY separates points, [x]A =φ1(φ(x)) follows.

Corollary 5.24.Let φ: (X,BX, μ) (Y,BY, ν) be a measure-preserving map between Borel probability spaces, and let A ⊆BY be a sub-σ-algebra.

Then

φμφx1A =νφ(x)A forμ-almost everyx∈X.

Proof.First notice that for anyf ∈L1(Y,BY, ν), Eν(fA)◦φis φ1A- measurable and

φ1A

Eν(fA)◦φdμ=

A

Eν(fA) dν

=

A

fdν

=

φ1A

f◦φdμ.

It follows that

Eν(fA)◦φ=Eμ(f◦φφ1A).

Thus forf ∈L(Y,BY),

fdνφ(x)A =Eν(fA) (φ(x))

=Eμ(f ◦φφ1A)(x)

=

f◦φdμφx1A

=

fd

φμφx1A

(all almost everywhere). Using a dense countable subset ofC(X) completes

the proof.

In the next result we will work with measurability on Borel subsets of compact metric spaces, without reference to a particular measure.

Lemma 5.25.Let X, Y, Z be Borel subsets of compact metric spaces X,Y and Z respectively, and let φZ : X Z and φY : X Y be measurable maps. Suppose that φZ is φY1(BY)-measurable. Then there is a measurable mapψ:Y →Z with φZ(x) =ψ◦φY(x)on X, as illustrated in Fig.5.4.

Fig. 5.4 The map constructed in Lemma5.25

This is related to Corollary 5.22, in that it allows us to draw the same conclusion that we can write the conditional measure μAx as a measurable functionνy on the image spaceY wheneverA =φ1BY.

Proof of Lemma5.25.DefineA =φY1(BY), which is countably-generated sinceBY is. Since the Borelσ-algebraBY ofY separates points,

[x]A =φY1(φY(x))

5.4 Algebras and Maps 149

forx∈X. By assumption, φZ isA-measurable, and henceφZ(x) =φZ(x) whenever [x]A = [x]A, or equivalently whenever φY(x) = φY(x). So we could define

ψ(y) =φZ(x)

whenever y = φY(x) for some x X, and use some fixed z0 Z to de- fine ψ(y) = z0 for y Y(X). However, it is not clear why this should define a measurable function, so instead we will defineψ:Y →Z by a lim- iting process. In order to do this we will cut the target space Z into small metric balls, and ensure that at each finite stage everything is appropriately measurable. For this we start with the additional assumption thatZ=Z is a compact metric space, and later show that this requirement can be removed.

Since Z is compact, there is a sequence (ξn) of finite Borel measurable partitions ofZ with the property that

σ(ξn)⊆σ(ξn+1)

forn1, and for which every element ofξn has diameter less than n1. We will define related partitionsξXn andξnY ofX andY. The first of these is defined by taking pre-images as follows. SinceφZ isA-measurable we get, for anyP ∈ξn, a set

PX=φZ1(P)∈A,

and hence a finite partitionξnX={PX |P ∈ξn} ⊆A ofX. This is illustrated in Fig.5.5.

Fig. 5.5 The partitionsξnonM(X) andξnXonX

We next define the partition ξnY. Note that in the construction of ξnY care needs to be taken, since the set φY(X) is not assumed to be mea-

surable. Since A = φY1BY, we can choose for every PX ξXn a set PY in BY with PX =φY1PY. Since the various sets PX ∈ξnX are disjoint, we can require the same disjointness for the sets PY. Indeed if sets P and Q in ξn are different, PX = φZ1P = φY1P, and QX = φZ1Q = φY1QY with QY, PY BY not disjoint, then replacing QY by QYPY will not change its properties but will ensure disjointness fromPY. Moreover, using a similar argument inductively we can also insist that Pn+1Y PnY when- everPn+1X ⊆PnXandPn+1X ∈ξn+1X ,PnX∈ξXn. The setsPY ∈BY forP∈ξnX, together with their common complementQn ∈BY, form a partitionξnY ofY. By construction,φ1Qn=∅and Qn+1⊇Qn for alln1. Write

Q=

m1

Qm

and define ψ(y) to be some fixed element z0 Z for any y Q. We de- fine ψ on YQ as the limit of the sequence of functions ψn : YQ Z defined as follows. For every PY ξYn, we choose some zP P ξn and define ψn(y) = zP for y PYQ. Clearly ψn : YQ Z is measurable, since the partitionξnY is measurable by construction. By construction of the partitions ξn, the diameters of the partition elementsP ∈ξn go to zero, so the functionψdefined by

ψ(y) = lim

n→∞ψn(y)

exists for ally ∈YQ; since it is a pointwise limit of a sequence of measur- able functions, the mapψis also measurable. Ify =φY(x) for somex∈X, then φZ(x) and ψn(y) will belong to the same element of ξn for all n, soφZ(x) =ψ(φY(x)) as required.

Assume now thatZ is only a Borel subset of a compact metric space Z.

The construction above can be used to define a measurable mapψ:Y →Z withφZ =ψ◦φY. Since

∅=φZ1ZZ

=φY1

ψ1ZZ we may replaceψby the measurable map

ψ(y) =

ψ(y) ifψ(y)∈Z, and z0∈Z if not,

for some fixed elementz0∈Z without affecting the fact thatφZ =ψ◦φY.

Dalam dokumen Ergodic Theory (Halaman 164-170)