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Inverse probability weighting identifies a causal mean

Statement

Assume AC for the conditional-expectation existence convention. Let P be a full-data law with a discrete or atomic treatment A, covariate random element L, observed outcome Y, and potential outcomes (Yb)b∈A with the countably discrete convention given by Potential outcomes and consistency. Fix an atom a with P(A=a)>0 and Ya∈L1(P). Assume consistency Y=YA, conditional exchangeability (Yb)b∈A⊥ ⁣ ⁣ ⁣⊥A∣σ(L), and positivity ea(L):=P(A=a∣σ(L))>0 almost surely. For Ia=1{A=a} and the observed law Q of (A,L,Y), the inverse-probability-weighted functional of Inverse probability weighting for a causal mean is well-defined and satisfies EQ ⁣[IaYea(L)]=EP[Ya]. Consequently, it identifies the population mean of Ya in the sense of Identifiability of an estimand. No uniform lower bound on ea is assumed. This is a population identity for the true propensity, not a finite-sample stability or estimated-weight result.

For countably discrete treatments, the supplied potential outcomes and global consistency use Potential outcomes and consistency; conditional exchangeability is the full-family sigma-algebra condition of Conditional exchangeability of potential outcomes. More generally, for a treatment in any measurable space with measurable singleton {a}, the same conclusion holds whenever the supplied integrable Ya is conditionally independent of A given σ(L) and 1{A=a}Y=1{A=a}Ya almost surely, with the same positive propensity. This atom-consistency formulation does not require a global measurable selection YA outside the target atom.

Facts & Assumptions

Given: AC, a probability space under P, a fixed treatment atom a, Ya∈L1(P), consistency Y=YA, conditional exchangeability (Yb)b∈A⊥ ⁣ ⁣ ⁣⊥A∣σ(L), and ea(L)>0 almost surely.

[A1]

The point-treatment setup uses potential outcomes and consistency as in Potential outcomes and consistency. For the full-family formulation, assume Y=YA, integrability of Ya, and conditional independence of the potential-outcome family from A given σ(L). For the general fixed-atom formulation, assume the atom-consistency and coordinate independence specified in the Statement; those are exactly the two consequences used below.

[A2]

The target is the causal mean relative to the causal model and observed law described by Identifiability of an estimand.

[F1]

The IPW functional is EQ[IaY/ea(L)], where ea=EQ[Ia∣σ(L)] and the weighted variable is required to be integrable. (Inverse probability weighting for a causal mean)

[F2]

For integrable Z⊥ ⁣ ⁣ ⁣⊥A∣G, E[1{A∈C}Z∣G]=E[1{A∈C}∣G]E[Z∣G]. (Conditional treatment-indicator factorization)

[F3]

A bounded G-measurable factor can be taken outside conditional expectation. (Taking out what is known)

[F4]

Integrals of a nondecreasing sequence of nonnegative measurable functions converge to the integral of their pointwise limit. (Monotone convergence for the integral)

[F5]

Dominated convergence gives L1 convergence under an integrable majorant and convergence of the corresponding integrals. (Dominated convergence)

[F6]

Conditional expectation preserves the expectation when conditioning down to the trivial sigma-algebra. (Tower property of conditional expectation)

[F7]

An estimand is a specified function on a statistical model. (Estimands on a statistical model)

[F8]

Equal observed sampling laws must give equal values of an identifiable estimand. (Identifiability of an estimand)

[F9]

Identifiability is equivalent to a unique factorization through the statistical model map. (Identifiability is constancy on observational classes)

[F10]

Conditional expectations are almost-sure classes of integrable measurable versions under AC. (Conditional expectation as an ae class)

[F11]

The expectation of an event indicator is its probability: E[1B]=P(B). (The expectation of an indicator is the probability of the event)

[F12]

Conditional independence is preserved by measurable maps of either variable. Thus full-family exchangeability implies independence of Ya and A given G, and independence of Ya implies that of ∣Ya∣. (Conditional-independence equivalences and preservation)

[F13]

For a measurable function of a random element, expectation equals its integral against that element's law; integrability of the composite implies integrability under the law. (Change of variables for expectation)

[F14]

Conditional-expectation versions of the same integrable variable agree almost surely. (Conditional expectation is unique almost surely)

Proof

1.1givenA1F1F6F10F11F13F14

Put G=σ(L), Ia=1{A=a}, ea=EP[Ia∣G], μa=EP[Ya∣G], and Hn=min⁡(n,1/ea) on {ea>0}, setting Hn=0 on the null complement. Let λ=PL=QL be the common covariate law. Since G=σ(L)={L−1(B):B∈S}, each real G-measurable version V factors as v(L): for each rational r choose Br∈S with {V<r}=L−1(Br), and put v(x)=inf⁡{r∈Q:x∈Br}, replacing nonfinite values by 0. Its rational sublevel sets make v measurable, and v(L)=V. Apply this to versions of the P- and Q-conditional propensities to obtain functions eˉa and e~a. By [F13] both are integrable under λ. For every measurable set B in that space, ∫Be~a dλ=Q(A=a,L∈B)=EP[Ia1{L∈B}]=∫Beˉa dλ. The difference is integrable and has zero integral over every B, so it and zero are conditional-expectation versions of zero given the full sigma-algebra on (L,S,λ). Uniqueness [F14] gives e~a=eˉa λ-almost everywhere. Thus the propensity used by [F1] agrees with the full-data propensity. By [F6] and [F11], P(A=a)=EP[Ia]=EP[ea]. Then Hn is bounded and G-measurable, Hn↑1/ea almost surely, and IaY=IaYa almost surely by global consistency or the stated atom-consistency. The conditional expectations exist by AC.

2.1A1F2F3F4F5F12step 1.1

Full-family exchangeability, or the stated coordinate independence directly, gives Ya⊥ ⁣ ⁣ ⁣⊥A∣G. By [F12], this also holds for ∣Ya∣, so [F2] gives E[Ia∣Ya∣∣G]=eaE[∣Ya∣∣G]. For each n, taking out the bounded factor Hn yields E[Ia∣Ya∣Hn]=E[eaHnE[∣Ya∣∣G]]. Monotone convergence [F4] on the left and dominated convergence [F5] on the right, since 0≤eaHn↑1 and E[∣Ya∣∣G]∈L1, give E[Ia∣Ya∣/ea]=E∣Ya∣<∞. Thus the observed weighted outcome is integrable.

3.1F2F3F5step 2.1

By [F3], [F2] also gives E[IaYa∣G]=eaμa. For each n, E[IaYaHn]=E[eaHnμa]. The left sides converge to E[IaYa/ea] by [F5] with integrable majorant Ia∣Ya∣/ea from step 2.1; the right sides converge to E[μa] by [F5] with majorant ∣μa∣. Hence E[IaYa/ea]=E[μa].

4.1A1F1F6F13step 1.1step 2.1step 3.1

By step 1.1 choose the common covariate-law representative eˉa and set the observed-coordinate ratio to zero on its λ-null nonpositive set. The change-of-variables identity [F13], first for the absolute value and then for the integrable signed function, shows that the Q-integrand in [F1] and its P observed-coordinate version have the same integral. Their common absolute integral is EP[Ia∣Ya∣/ea], finite by step 2.1 and IaY=IaYa almost surely, so [F1] is well-defined. The same identity, atom-consistency, step 3.1, and the tower property [F6] give EQ[IaY/ea(L)]=EP[IaYa/ea]=EP[Ya].

5.1A2F1F7F8F9step 1.1step 4.1construct∎

Let Θa be the class of full-data laws on the fixed measurable spaces for the variables in the applicable formulation of the Statement that satisfy its integrability, consistency, conditional-exchangeability (or atom-specific independence), and positivity assumptions. Define ψa(P)=EP[Ya] and the observation map O(P)=LP(A,L,Y)=Q, the pushforward of P under (A,L,Y). Step 4.1 proves for every P∈Θa that ψa(P)=ΨIPW(O(P);a). This factor is a function of the observed law alone, with its conditional propensity class determined by that law as in step 1.1; [F7]–[F9] therefore give identifiability on this model.

Remarks

Strict positivity is required at each target covariate stratum but need not be bounded away from zero. Near-positivity can make the integrand very variable, as the examples page shows. No finite-sample stability, estimated-propensity consistency, or validity after weight truncation follows from this identity. Continuous-treatment density weights are outside this theorem's scope.

Depends on

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