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Backdoor adjustment identifies an interventional law

Statement

Assume AC and a finite Markovian SCM on a finite DAG G. Let A and Y be distinct observed vertices, with A a countable-valued treatment and Y an observed standard-Borel outcome. Let L be an observed finite vector of standard-Borel vertices whose vertex set is disjoint from {A,Y} and contains no descendant of A. Fix an atom a with P(A=a)>0. Suppose (i) L d-separates A and Y in GA‾ and (ii) a regular conditional propensity ea(L)=P(A=a∣L) is strictly positive PL-almost surely. Then for every Borel set B in the state space of Y, P(Ya∈B)=∫P(Y∈B∣A=a,L=l) PL(dl). The right side depends only on the observed law. Thus the law of Ya is an identifiable estimand on any statistical model consisting of such SCMs with the same observed variables. If Y is real and Ya is integrable, applying the identity to bounded truncations and taking limits gives E[Ya]=∫E(Y∣A=a,L=l) PL(dl). For a continuous treatment, the corresponding regular conditional formula is identified only for PA-almost every a; this theorem makes no pointwise claim at a null treatment value.

Facts & Assumptions

Given: The SCM, observed variables, atom a, backdoor separation, and positivity stated above.

[F1]

The graph criterion implies Ya⊥A∣L in the Markovian SCM. The backdoor criterion implies conditional exchangeability

[F2]

Under AC, standard-Borel variables have regular conditional laws and joint laws disintegrate in either declared coordinate direction. Existence of regular conditional distributions for standard borel targets, Disintegration of a joint law on standard borel spaces

[F3]

On {A=a} the structural response agrees with the factual outcome: Y=Ya. Recursive structural causal models on finite DAGs

[F4]

Proof

technique · conditional exchangeability, consistency, and positivity give the adjustment functional

Given: The hypotheses in the statement.

1.1F1F2given

By [F1], Ya and A are conditionally independent given L. By [F2] take regular conditional laws of Ya given L and given (A,L). The conditional-independence identity implies that, for PA,L-almost every (a′,l), the latter law equals the former law at l. Since a is an atom with ea(l)>0 for PL-almost every l, the measure PL∣A=a is equivalent to PL: its density with respect to PL is ea(l)/P(A=a), which is positive and integrates to one. Hence the conditional-law equality at A=a holds for PL-almost every l.

2.1givenF3step 1.1algebra

On the event A=a, the factual structural recursion and the recursion with the A equation replaced by a agree at A. Induction down the fixed topological order shows that they agree at every descendant, in particular Y=Ya. Therefore the conditional law of Ya given A=a,L=l equals that of Y given A=a,L=l for PL-almost every l. Combining with step 1.1 identifies the conditional law of Ya given L=l with the observed conditional law in the formula.

3.1step 2.1F2F4algebra∎

Disintegrating the joint law of (Ya,L) by [F2] gives P(Ya∈B)=∫P(Ya∈B∣L=l)PL(dl). Substitute the equality from step 2.1 to obtain the displayed formula. If two SCM parameter values induce the same observed law, the integrand kernel and PL agree outside their common null sets; positivity makes those sets null for the target integral. Hence the right side, and so the estimand, is constant on each observational-equivalence class by [F4]. The real-valued expectation formula follows by applying the distribution identity to bounded truncations of Y and using integrability to pass to the limit.

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