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Front-door adjustment identifies an interventional mean

Statement

Assume AC and a finite Markovian SCM with pairwise distinct observed vertices A,M,Y, where A is a countable-valued treatment, M a standard-Borel mediator, and Y a real outcome. Fix an atom a with P(A=a)>0. Suppose in the full DAG: (i) M lies on every directed path from A to Y; (ii) A and M are d-separated by the empty set in GA‾; and (iii) A d-separates M and Y in GM‾. Write μa=P(M∈⋅∣A=a) and, for every positive-probability treatment atom a′, write μa′=P(M∈⋅∣A=a′). Assume the nested-law support condition μa≪μa′for every a′ with P(A=a′)>0, and absolute integrability of the nested conditional means: ∫ ⁣∫E(∣Y∣∣M=m,A=a′) PA(da′) μa(dm)<∞. Then E[Ya]=∫P(dm∣A=a)∫E(Y∣M=m,A=a′) PA(da′). The right side is determined by the observed law, so the interventional mean is identifiable on any statistical model of SCMs satisfying these assumptions. For a discrete mediator, the support condition says that every mediator value having positive probability under A=a also has positive probability under every positive-probability treatment atom. These are sufficient conditions only. For non-atomic treatment values, regular conditional formulas are determined only PA-almost everywhere; this item makes no pointwise claim at a null treatment value.

Facts & Assumptions

Given: The SCM, three graph conditions, target atom, nested-law support, and absolute-integrability conditions in the statement.

[F1]

The front-door graph conditions give Ma⊥A, M⊥UIY∣A, Ma⊥UIY, and Ya=YMa, where IY is the finite set of exogenous coordinates defined in the helper. Counterfactual identities under the front-door conditions

[F3]

Integration of a jointly measurable function against a probability kernel is measurable, and Fubini applies on the resulting finite product probability spaces. Measure kernel and probability kernel, Measurability of integration against a kernel, Fubini's theorem for L^1 functions on a sigma-finite product

[F4]

Conditional expectation has the tower property; increasing nonnegative approximations and monotone convergence justify the integrable limit operations. Conditional expectation given a sigma algebra, Tower property of conditional expectation, Every nonnegative measurable function is the increasing limit of simple measurable functions, Monotone convergence for the integral, The Axiom of Choice

Proof

technique · represent the outcome response by its exogenous coordinates, use conditional independence to recover its observed conditional kernel, and integrate that kernel against the intervention mediator law

Given: The hypotheses in the statement.

1.1F1F2F3F4givenconstruct

Let IY be as in [F1], let UY=∏v∈IYEv, and let ν be the law of UIY. Recursion under do(M=m) gives a jointly measurable function F:SM×UY→R with Ym=F(m,UIY). Under the factual equations, the same recursion gives Y=F(M,UIY), because UM enters only the equation for M and all other exogenous coordinates that can affect Y after fixing M lie in IY. For each supported atom a′, let νa′(D)=P(UIY∈D∣A=a′). By [F1], conditional independence gives P((M,UIY)∈⋅∣A=a′)=μa′⊗νa′. Thus, for every Borel set B⊆R, the measurable function λa′(m,B)=∫1B(F(m,u)) νa′(du) satisfies, for each Borel mediator set D, P(Y∈B,M∈D∣A=a′)=∫Dλa′(m,B) μa′(dm). It is therefore a regular conditional law of Y given (M,A=a′); uniqueness in [F2] identifies it with the observed conditional kernel μa′-almost everywhere. Applying this identity to bounded truncations and then using [F4] gives ∫∣F(m,u)∣ νa′(du)=E(∣Y∣∣M=m,A=a′) for μa′-almost every m.

2.1step 1.1F2F4givenalgebra

For each positive-probability atom a′, the support assumption μa≪μa′ transfers the full-measure identity from step 1.1 to a μa-full set. The treatment support is countable, so the intersection of these sets is still μa-full. The integrability hypothesis and the nonnegative identity in step 1.1 imply ∫ ⁣∫∣F(m,u)∣ νa′(du) PA(da′) μa(dm)<∞. Since A is countable-valued, the law of UIY is the mixture ν=∫νa′PA(da′). Hence ∫ ⁣∫∣F(m,u)∣ ν(du) μa(dm)<∞, and the conditional mean kernel has the observed-law representation ∫F(m,u) ν(du)=∫E(Y∣M=m,A=a′) PA(da′) for μa-almost every m.

3.1F1step 2.1F3givenalgebra

By [F1], Ya=YMa=F(Ma,UIY) and Ma is independent of UIY. The integrability from step 2.1 permits Fubini [F3], so E[Ya]=∫ ⁣∫F(m,u) ν(du) PMa(dm). Also [F1] gives Ma⊥A, and consistency on {A=a} gives PMa=P(M∈⋅∣A=a)=μa. Substituting step 2.1 proves the displayed front-door formula.

4.1givenF2F5step 3.1∎

The right side of the formula uses only the observed law of (Y,M,A). Conditional-mean versions agree μa-almost everywhere by step 2.1 and the domination assumption. Therefore any two SCM parameter values with the same observed law give the same target mean, which is identifiability by [F5].

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