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  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
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Parent dependence persists under nondescendant conditioning

Statement

Assume Countable Choice, or suppose the specified noise densities are Borel measurable. Let X follow a finite additive-noise model with a strictly positive joint density and continuous structural functions that are causally minimal in each parent coordinate. For positive joint densities, write Y⊥dA∣Z when the conditional-density factorization pY,A,Z(y,a,z)pZ(z)=pY,Z(y,z)pA,Z(a,z) holds almost everywhere. For every edge i→j and every set S such that pa⁡(j)∖{i}⊆S⊆nd⁡(j)∖{i}, the density conditional-independence factorization Xj⊥dXi∣XS fails.

Facts & Assumptions

Given: A finite ANM with positive joint density, continuous parent-coordinate functions, and causal minimality.

[F1]

Every parent input is essential: for each edge i→j, fj is nonconstant in the i-coordinate for some setting of the other parents; noises are independent and have positive densities. Continuous additive-noise models on finite DAGs

[F2]

For Borel noise densities (supplied, or chosen under Countable Choice without changing the laws), the joint density is the positive Borel product pX(x)=∏kqk(xk−fk(xpa⁡(k))). Marginal densities are obtained by integrating this formula, and a conditional density at a positive finite marginal-density value is the corresponding ratio. Positive joint density of a finite additive-noise model

[F3]

For every vertex j, Nj is independent of any vector of nondescendants. An ANM noise is independent of every set of nondescendants

Proof

Given: Fix an edge i→j and a set S in the range in the Statement. Put P=pa⁡(j)∖{i} and Q=S∖P.

1.1givenF1F2F3

Use the supplied Borel noise densities, or their positive finite Borel versions from [F2] under Countable Choice. Work with their Borel shifted-noise product and its integrated marginals; changing density versions does not change an almost-everywhere conditional-independence factorization. Every variable in {i}∪P∪Q is a nondescendant of j. By [F3], Nj is independent of the vector (Xi,XP,XQ). Conditional on (Xi=x,XP=p,XQ=q), the structural equation therefore gives the density pXj∣Xi,XP,XQ(y∣x,p,q)=qj(y−fj(p,x)) for almost every (x,p,q,y). This density does not depend on q, so the joint conditional density of (Xj,XQ) given (Xi,XP) factors; hence Xj⊥dXQ∣(Xi,XP).

1.2givenF1F2F3algebra

Suppose, for contradiction, that Xj⊥dXi∣XP. Since Nj is independent of the parent vector (Xi,XP), its conditional density is qj(y−fj(p,x)). The assumed factorization says this density is independent of x for almost every p and almost every x. The conditional density of Xi given XP=p is positive for almost every x at almost every p with 0<pP(p)<∞, because the full joint density is strictly positive. Therefore, for almost every such p, for almost every pair x,x′, the two translates qj(y−fj(p,x)) and qj(y−fj(p,x′)) agree for almost every y.

2.1step 1.2F1F2algebra

A positive integrable density cannot have a nonzero period: if qj(y−a)=qj(y−b) almost everywhere with a≠b, then qj repeats on every translate of an interval of length ∣a−b∣; that interval has positive integral, so the integral over the disjoint translates is infinite, contradicting ∫qj=1. Thus step 1.2 forces fj(p,x)=fj(p,x′) for almost every pair x,x′ and almost every p. Continuity of fj extends this constancy to every setting of the other parent coordinates: any two unequal values would persist on open neighborhoods of positive Lebesgue measure. This contradicts [F1], so Xj̸⊥dXi∣XP.

3.1step 1.1step 2.1F2algebra∎

If Q is empty, S=P and step 2.1 is the required conclusion. Otherwise, suppose Xj⊥dXi∣XP,Q. By the conditional-density equality in step 1.1 and this supposition, for almost every (p,y) one has pXj∣Xi=x,XP=p(y)=pXj∣XP=p,XQ=q(y) for almost every pair (x,q). The left side depends only on x and the right side only on q; by Fubini, each is therefore almost everywhere constant in its varying coordinate. Hence Xj⊥dXi∣XP, contradicting step 2.1. Thus the factorization given XS fails.

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