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Missingness weights and sensitivity

1 · Prerequisites

2 · Summary

This page defines the response-probability weighted sample mean, proves the population inverse-weighting identity under the explicit MAR conditional independence condition, and specifies a location-shift pattern-mixture sensitivity family. The identity assumes the true positive response probability and an integrable outcome. It does not establish finite-sample stability, estimated-weight inference, or a joint treatment and response weighting result.

The sensitivity function constrains the full conditional distribution among nonrespondents. It is a modeling assumption, not a consequence of the observed data. Its mean target requires a separate integrability condition, and any range over sensitivity values is not itself a confidence interval.

3 · Logical flowchart

4 · Definitions, theorems and proofs

LemmaStatement: AI-adaptedProof: AI-generatedprecheck passjudge pass (gpt-6-luna)Open item page →

Conditional-independence factorization for integrable outcomes

Statement

Assume AC. Let (Ω,F,P) be a probability space, let G⊆F be a sub-sigma-algebra, let R be a random variable taking values in {0,1}, and let Y be a real integrable random variable. If R and Y are conditionally independent given G, then for every Borel function φ:R→R such that φ(Y) is integrable, E[Rφ(Y)∣G]=E[R∣G]E[φ(Y)∣G]almost surely.

Facts & Assumptions

Given: AC, the probability space and sub-sigma-algebra above, R∈{0,1}, Y∈L1(P), R⊥ ⁣ ⁣ ⁣⊥Y∣G, and a Borel φ with Z=φ(Y)∈L1(P).

[F1]

Conditional independence means the conditional product identity for every pair of bounded measurable real functions. (Conditional independence given a sigma-algebra)

[F2]

A conditional-expectation version is measurable, integrable, and satisfies the defining event-integral identity. (Conditional expectation given a sigma algebra)

[F3]

Under AC, conditional expectation is linear and order-preserving, and E∣E[U∣G]∣≤E∣U∣ for every real U∈L1(P). (Basic algebra and order properties of conditional expectation)

[F4]

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

[F5]

For a real measurable Z, integrability means E∣Z∣<∞. (Integrable real and complex functions, and their integrals)

[F6]

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

[A1]

AC is assumed to define conditional independence and guarantee existence of the conditional-expectation classes used here. (The Axiom of Choice, Conditional independence given a sigma-algebra, Basic algebra and order properties of conditional expectation)

Proof

1.1givenA1F1F2

For m≥1, put Zm=max⁡(−m,min⁡(Z,m)). The functions z↦max⁡(−m,min⁡(φ(z),m)) and r↦r are bounded and measurable, so [F1] gives E[RZm∣G]=E[R∣G]E[Zm∣G], with the conditional-expectation versions interpreted by [F2].

2.1givenF3F4F5F6step 1.1∎

The truncations satisfy Zm→Z in L1: ∣Z−Zm∣≤∣Z∣1{∣Z∣>m}, and [F4] applied to ∣Z∣1{∣Z∣≤m}↑∣Z∣ makes the tail integrals tend to zero, using integrability [F5] and expectation as integral [F6]. By [F3], conditional expectation is an L1 contraction; since 0≤E[R∣G]≤1, both sides of the identity in step 1.1 converge in L1 to the corresponding sides for Z. Uniqueness of the L1 limit proves the claimed equality.

Source notes

The cited notes define conditional independence only for bounded measurable test functions. The truncation argument above supplies the integrable extension used in this item.

AlgorithmAlgorithm: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Response-probability weighting for a sample mean

Definition

Let (X,A) be a measurable covariate space and let n≥1. In the one-outcome full/observed-data convention of Full and observed data under a missingness pattern, Xi∈X is observed for every unit, Ri∈{0,1} indicates whether the real outcome Yi is observed, and the encoded input stores Zi=Yi when Ri=1 and the placeholder Zi=0 when Ri=0. The mask Ri distinguishes the placeholder from an observed zero; it is not an imputation or a replacement of the missing full-data value. Let π:X→(0,1] be a supplied, known, measurable response-probability function, with π(xi)>0 for every record in the input.

Input: n, records (xi,ri,zi)i=1n satisfying the stated conventions, and the function π.

Procedure: For each record use weight 1/π(xi) when ri=1 and weight zero when ri=0. Return the unnormalized Horvitz–Thompson weighted mean μ^HT=1n∑i=1nziπ(xi).

The procedure takes the true known response probabilities as input. Substituting fitted probabilities is a different procedure; this definition makes no finite-sample stability or estimated-weight inference claim. The weighting convention is the one used for a single response indicator; no joint treatment/response weight is defined here.

TheoremStatement: Literature-sourcedProof: AI-generatedprecheck passjudge pass (gpt-6-luna)Open item page →

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.

DefinitionDefinition: AI-adaptedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Location-shift pattern-mixture sensitivity function

Definition

Assume AC. Let X take values in a standard-Borel space X, let Y be real-valued, and let R∈{0,1} indicate response in the one-outcome full/observed-data setup of Full and observed data under a missingness pattern. Suppose P(R=1)>0, P(R=0)>0, and the covariate laws overlap in this direction: for every measurable A⊆X, P(X∈A∣R=1)=0 implies P(X∈A∣R=0)=0. Under the respondent law P(⋅∣R=1), choose a conditional law K1(x,⋅) of Y given X=x; standard-Borel disintegration supplies such a probability kernel under AC (Disintegration of a joint law on standard borel spaces, Conditional law given a random element). The overlap condition makes the respondent version relevant almost surely under the nonrespondent covariate law.

A location-shift pattern-mixture sensitivity function is a measurable Δ:X→R for which the nonrespondent conditional law is specified by K0Δ(x,B)=∫R1B(y+Δ(x))K1(x,dy) for every Borel set B⊆R, on the covariate support of nonrespondents. This is the full conditional distribution restriction Y∣(X=x,R=0)=dY1+Δ(x) for Y1∼K1(x,⋅), not merely a restriction on conditional means. For each x, K0Δ(x,⋅) is the pushforward of K1(x,⋅) under the measurable translation y↦y+Δ(x), hence is a probability measure; its evaluations are measurable in x by kernel integration because (x,y)↦1B(y+Δ(x)) is measurable (Measure kernel and probability kernel, Measurability of integration against a kernel). The relation specifies the missing conditional law while leaving the respondent conditional law fixed. A finite mean target additionally requires integrability under the resulting full-data law; the definition alone does not assert that moment condition.

In this specified family, Δ=0 gives equality of the respondent and nonrespondent conditional laws. This does not make equality of conditional means alone equivalent to MAR in a general full-data model; equality of means need not imply equality of distributions. Values where no respondents occur are outside the definition because K1 is unavailable there, and a pattern with no nonrespondents requires no sensitivity function.

The formal one-outcome MCAR/MAR/MNAR taxonomy for this pair is supplied by MCAR, MAR, and MNAR relative to an observation pattern. The location-shift relation above is the selected sensitivity model within that taxonomy; it does not claim that all MNAR laws are location shifts.

Source notes

National Research Council Chapter 5 introduces sensitivity parameters through differences between respondent and nonrespondent distributions and illustrates a mean-shift parameter. This item deliberately specifies the stronger full-distribution location-shift model shown above; the cited source supports the modeling framework, not a theorem that this particular translation restriction is empirically true.

5 · Examples, counterexamples and false statements

None yet.

Sources