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Basic algebra and order properties of conditional expectation

Statement

Assume AC for existence. For real X,Y∈L1(P) and a,b∈R, E[aX+bY∣G]=aE[X∣G]+bE[Y∣G]. Conditional expectation is positive, preserves order and constants, satisfies E(E[X∣G])=EX, and ∣E[X∣G]∣≤E[∣X∣∣G] almost surely. Also X<Y almost surely implies E[X∣G]<E[Y∣G] almost surely.

Facts & Assumptions

Given: AC, a probability space, a sub-sigma-algebra G, real integrable X,Y and real scalars a,b; for the strict clause assume X<Y almost surely.

[F1]

Under AC the conditional class exists and each version has the defining event integrals. (Conditional expectation as an ae class)

[F2]

Versions with the same defining data agree almost surely. (Conditional expectation is unique almost surely)

[F3]

Integrability and integrals are preserved by finite linear combinations. (The Lebesgue integral is linear on L1(μ))

[F4]

A nonnegative measurable function has zero integral exactly when it is zero almost everywhere. (A nonnegative measurable function has integral 0 exactly when it vanishes almost everywhere)

[F5]

Linear combinations, positive and negative parts, absolute values and discrepancy sets are measurable; restricting a nonnegative measurable function to a measurable event preserves measurability. (Closure properties of measurable functions used by the integral)

[F6]

Almost-everywhere equal integrable functions have equal integrals on every measurable event. (Two integrable functions are equal almost everywhere exactly when all of their indefinite integrals agree)

Proof

technique · direct
1.1F1F2F3F5

Choose versions U=E[X∣G] and V=E[Y∣G]. The function aU+bV is G-measurable and integrable. For every A∈G, ∫A(aU+bV)=a∫AX+b∫AY=∫A(aX+bY). It is a version of the left side, so uniqueness proves linearity.

2.1step 1.1F1F3F4F5F6

If X≥0 almost surely, its positive part X+ is measurable by [F5], integrable because X+≤∣X∣, and equals X almost surely. Set A={U<0}∈G. By [F6] and [F1], 0≤∫AX+=∫AX=∫AU. The measurable integrable function U−=max⁡{−U,0} equals −U on A and zero off A, so [F3] gives ∫AU=−∫U−≤0. Thus ∫U−=0; [F4] gives U−=0 almost surely and hence P(A)=0. For X≤Y almost surely apply this positivity result to Y−X and use step 1.1, proving order preservation.

3.1step 1.1step 2.1F1F2

The constant function c is integrable, G-measurable, and has its own event integrals, so E[c∣G]=c by uniqueness. Testing A=Ω in [F1] gives EU=EX. Finally −∣X∣≤X≤∣X∣ and steps 1.1–2.1 give −E[∣X∣∣G]≤U≤E[∣X∣∣G]. Hence ∣U∣≤E[∣X∣∣G] and E∣U∣≤E∣X∣.

4.1step 1.1step 2.1F1F4F5F6∎

If W=Y−X>0 almost surely, let T=E[W∣G]≥0 almost surely by step 2.1. On A={T=0}∈G, [F1] gives ∫AW=∫AT=0. The positive part W+ is measurable and integrable, and W+=W almost surely; [F6] therefore gives ∫W+1A=∫AW=0. The integrand is pointwise nonnegative and measurable by [F5], so [F4] gives W+1A=0 almost surely. Since W+>0 off a null set, this forces P(A)=0. Together with P(T<0)=0 this gives T>0 almost surely; step 1.1 identifies T=V−U almost surely.

Source notes

Durrett Lemma 4.1.1 and Theorem 4.1.9(a)–(b), printed pp.206,210–211; van der Vaart Lemma 1.9(i),(iii),(iv), printed p.4. The strict almost-sure statement is derived by the zero-event argument, not attributed to a counterexample.

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