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Parent dependence persists under nondescendant conditioning
Statement
Assume Countable Choice, or suppose the specified noise densities are Borel measurable. Let 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 when the conditional-density factorization holds almost everywhere. For every edge and every set such that the density conditional-independence factorization fails.
Statement references
Facts & Assumptions
Given: A finite ANM with positive joint density, continuous parent-coordinate functions, and causal minimality.
Every parent input is essential: for each edge , is nonconstant in the -coordinate for some setting of the other parents; noises are independent and have positive densities. Continuous additive-noise models on finite DAGs
For Borel noise densities (supplied, or chosen under Countable Choice without changing the laws), the joint density is the positive Borel product . 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
For every vertex , is independent of any vector of nondescendants. An ANM noise is independent of every set of nondescendants
Proof
Given: Fix an edge and a set in the range in the Statement. Put and .
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 is a nondescendant of . By [F3], is independent of the vector . Conditional on , the structural equation therefore gives the density for almost every . This density does not depend on , so the joint conditional density of given factors; hence .
Suppose, for contradiction, that . Since is independent of the parent vector , its conditional density is . The assumed factorization says this density is independent of for almost every and almost every . The conditional density of given is positive for almost every at almost every with , because the full joint density is strictly positive. Therefore, for almost every such , for almost every pair , the two translates and agree for almost every .
A positive integrable density cannot have a nonzero period: if almost everywhere with , then repeats on every translate of an interval of length ; that interval has positive integral, so the integral over the disjoint translates is infinite, contradicting . Thus step 1.2 forces for almost every pair and almost every . Continuity of 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 .
If is empty, and step 2.1 is the required conclusion. Otherwise, suppose . By the conditional-density equality in step 1.1 and this supposition, for almost every one has for almost every pair . The left side depends only on and the right side only on ; by Fubini, each is therefore almost everywhere constant in its varying coordinate. Hence , contradicting step 2.1. Thus the factorization given fails.
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Sources
- Jonas Peters, Joris Mooij, Dominik Janzing, and Bernhard Schölkopf, Causal Discovery with Continuous Additive Noise Models, Appendix A.10, Lemma 38 and Proposition 17 (standard reference, not scraped)
- Jonas Peters, Dominik Janzing, and Bernhard Schölkopf, Elements of Causal Inference, §4.1.4 and §7.2 (standard reference, not scraped)