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Inverse response-probability weighting identifies the mean under MAR

Statement

Assume AC. Let (Ω,F,P) be a probability space, X a fully observed random element, G=σ(X), R∈{0,1} the response indicator (R=1 exactly when the real full-data outcome Y is observed, under the one-outcome convention of Full and observed data under a missingness pattern), and Y∈L1(P). Suppose R and Y are conditionally independent given G, the MAR condition in the assigned one-outcome, fully observed-X formulation. Let π be a chosen version of E[R∣G] and assume π>0 almost surely on the target law. Define RY/π to be zero on the null set where π=0. Then RY/π∈L1(P) and E ⁣[RYπ]=E[Y].

Here π is the true response probability, not a fitted estimate. This is a population identity; by itself it gives no finite-sample stability or estimated-weight inference result.

Facts & Assumptions

Given: AC, the probability space and random elements above, Y∈L1(P), R∈{0,1}, R⊥ ⁣ ⁣ ⁣⊥Y∣G, π=E[R∣G], and π>0 almost surely.

[L1]

Under conditional independence, E[Rφ(Y)∣G]=E[R∣G]E[φ(Y)∣G] for every Borel φ with φ(Y) integrable. (Conditional-independence factorization for integrable outcomes)

[F1]

Conditional-expectation versions are measurable and integrable and have the defining event integrals. (Conditional expectation given a sigma algebra)

[F2]

Conditional expectation is positive, preserves order and constants, and preserves the unconditional expectation. (Basic algebra and order properties of conditional expectation)

[F3]

Assume AC. For H⊆G and integrable U, E[E[U∣G]∣H]=E[U∣H] almost surely. (Tower property of conditional expectation)

[F4]

Increasing nonnegative measurable functions pass to the limit under the integral. (Monotone convergence for the integral)

[F5]

The expectation of an integrable real random variable is its Lebesgue integral. (Expectation of a nonnegative or integrable random variable)

[A1]

AC is assumed for conditional independence, conditional-expectation existence, and the tower property used here. (The Axiom of Choice, Conditional independence given a sigma-algebra, Basic algebra and order properties of conditional expectation, Tower property of conditional expectation)

Proof

1.1givenA1F1F2F4L1construct

Let G=σ(X) and choose the stated version π=E[R∣G]. By [F2], 0≤π≤1 almost surely, so replacing it by min⁡(1,max⁡(0,π)) gives a G-measurable version with 0≤π≤1 everywhere. For each nonnegative S∈{∣Y∣,Y+,Y−}, choose a G-measurable version US of E[S∣G], replace it by max⁡(US,0), and set it equal to zero on {π=0}. Positivity [F2] and π>0 almost surely show these changes are on G-measurable null sets, so each US remains a version by [F1]; it is pointwise nonnegative and vanishes on {π=0}. On {π>0} set qm=min⁡(m,1/π) and set qm=0 on {π=0}. For fixed m, the bounded G-measurable functions qm,n=2−n⌊2nqm⌋ are simple, nonnegative, and increase to qm. For any such S, [F1] gives E[qm,nRS]=E[qm,nE[RS∣G]] by summing the event-integral identities over the level sets of qm,n. Applying [L1] with φ(y)=∣y∣, y+, or y−, then using [F4] on the increasing nonnegative products as n→∞, yields E[qmRS]=E[qmπUS].

2.1givenF1F2F3F4F5step 1.1

As m→∞, qmRS↑RS/π under the stated zero convention. On {π>0}, qmπUS=min⁡(mπ,1)US↑US; on {π=0} both sides are zero by the representative chosen in step 1.1. Thus qmπUS↑US pointwise. By [F4], the equalities in step 1.1 pass to these limits. The tower property [F3] with H={∅,Ω} gives E[US∣H]=E[S∣H]; by the defining event-integral property [F1], conditioning on this trivial sigma-algebra yields the constant unconditional expectation. Thus E[US]=E[S], with [F5] identifying these finite expectations with their integrals. This holds for each of S=∣Y∣,Y+,Y−. In particular E∣RY/π∣=E∣Y∣<∞.

3.1F5step 2.1algebra∎

Subtracting the finite identities for Y+ and Y− from step 2.1 is legitimate by the absolute-integrability conclusion there. Since Y=Y+−Y−, this gives E[RY/π]=E[Y].

Remarks

The proof uses the true conditional response probability and the explicit conditional-independence hypothesis. If π is estimated, or if treatment and observation are weighted jointly, a separate sampling or joint/sequential law and its own positivity and proof are required. Strict positivity alone does not bound the weights; the companion example exhibits this boundary.

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