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Additive-noise causal discovery and identifiability — Examples

1 · Prerequisites

2 · Logical flowchart

3 · Definitions, theorems and proofs

None yet.

4 · Examples, counterexamples and false statements

ExampleConstruction: AI-generatedVerification: AI-generatedOpen item page →

Latent confounding can mimic an observed ANM direction

Example

Assume the Axiom of Choice. Let U,ϵX,ϵY be mutually independent standard normal random variables. In Model A, set U=NU, X=U+ϵX, and Y=U+ϵY, with U latent and X,Y observed. In Model B, let Z1,Z2 be independent standard normal variables, set X=2Z1, E=3/2Z2, and Y=X/2+E, with both vertices observed. In each model the observed vector (X,Y) has density p(x,y)=12π3exp⁡ ⁣(−x2−xy+y23). Under do(X=1), Model A gives Y=U+ϵY with density 12πe−y2/4, while Model B gives Y=1/2+E with density 13πe−(y−1/2)2/3. The two intervention densities differ at y=1/2, so the same observational law is compatible with different causal effects when a latent common cause is allowed.

Remarks

In the diagram, circles denote variables and arrows denote direct structural inputs. The dashed vertex U is latent in Model A, so only X and Y are observed there. Model B has the observed edge X→Y. The diagrams show the two model graphs; the density and intervention calculations below prove the claimed observational and interventional comparisons.

\begin{tikzpicture}[>=stealth]
  \node[draw,circle,dashed] (u) at (0,0) {$U$};
  \node[draw,circle] (xa) at (2,1) {$X$};
  \node[draw,circle] (ya) at (2,-1) {$Y$};
  \draw[->] (u) -- (xa);
  \draw[->] (u) -- (ya);
  \node at (1,-2) {Model A};
  \node[draw,circle] (xb) at (4,0) {$X$};
  \node[draw,circle] (yb) at (6,0) {$Y$};
  \draw[->] (xb) -- (yb);
  \node at (5,-1) {Model B};
\end{tikzpicture}

Facts & Assumptions

Given: Assume AC. Use the standard normal density ϕ(t)=(2π)−1/2e−t2/2 and the independent noises specified in the Example.

[A1]

Assume AC for the standard-normal law; AC implies countable choice (ACω), which is the additional interface used by normalization and Lebesgue-change suppliers. The Axiom of Choice, The Axiom of Countable Choice (ACω), AC implies DC implies countable choice

[F1]

The finite recursive SCM convention defines latent vertices, observed marginals, and do(XI=a) by replacing only the intervened equations. Recursive structural causal models on finite DAGs

[F3]

The Gaussian integral is ∫Re−t2 dt=π. The Gaussian integral ∫−∞∞e−x2 dx=π

[F4]

For a finite ANM on fully observed vertices, the joint density is the product of its shifted noise densities. Continuous additive-noise models on finite DAGs, Positive joint density of a finite additive-noise model

[F5]

Nonnegative product integrals may be marginalized in either coordinate order. Tonelli's theorem for nonnegative measurable functions on a sigma-finite product

Verification

Given: The two SCMs and standard normal densities in the Example.

1.1givenA1F3F4F5algebraconstruct

Under AC [A1], treat the full Model A vector (U,X,Y) as an ANM with noises (NU,ϵX,ϵY). By [F4]–[F5], its density is ϕ(u)ϕ(x−u)ϕ(y−u); marginalizing the latent U gives pA(x,y)=∫Rϕ(u)ϕ(x−u)ϕ(y−u) du. Completing the square, u2+(x−u)2+(y−u)2=3(u−x+y3)2+23(x2−xy+y2). Thus [F3] and the substitution t=3/2 (u−(x+y)/3) give pA(x,y)=12π3exp⁡ ⁣(−x2−xy+y23).

1.2givenA1F2F4algebra

The scaled standard normal variables in Model B have densities q2(x)=12πe−x2/4 and q3/2(e)=13πe−e2/3 by [F2]. The Model B equation is an ANM, so [F4] gives pB(x,y)=q2(x)q3/2(y−x/2)=12π3exp⁡ ⁣(−x2−xy+y23), where the last equality follows by expanding x2/4+(y−x/2)2/3=(x2−xy+y2)/3. Hence pA=pB pointwise.

2.1givenA1F1F2F3step 1.1step 1.2algebra∎

Under do(X=1) in Model A, [F1] replaces only the equation for X; the unchanged Y equation remains Y=U+ϵY. Its density is the convolution ∫ϕ(u)ϕ(y−u) du=12πe−y2/4, by completing the square and [F3]. In Model B the intervention gives Y=1/2+E, whose density is 13πe−(y−1/2)2/3 by [F2]. At y=1/2 the second density is larger than the first by the factor 23e1/16>1, so the intervention laws differ although the observational densities agree.

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A reversible linear-Gaussian additive-noise model

Example

Assume AC. Let X,N be independent standard normal random variables and set Y=X+N. The forward model Y=X+N is an additive-noise model, and the same joint law also has the reverse representation X=12Y+M,M:=X−N2, where M is independent of Y. Indeed, the joint density of (Y,M) is pY,M(y,m)=12πexp⁡ ⁣(−y24−m2)=(12πe−y2/4)(1πe−m2). The forward structural function f(x)=x and the two Gaussian log densities satisfy the differential equation in Condition 19 at every point of its nonzero domain, so Condition 19 fails. Thus this reversible case lies outside the bivariate identifiability theorem's hypothesis.

Facts & Assumptions

Given: Assume AC and take independent X,N∼N(0,1) with standard normal density ϕ(t)=(2π)−1/2e−t2/2.

[A1]

AC is the Axiom of Choice and implies countable choice (ACω), the additional axiom interface used by the normal-density and linear-change-of-variables suppliers. The Axiom of Choice, The Axiom of Countable Choice (ACω), AC implies DC implies countable choice

[F1]

The standard normal law has density ϕ, and its affine images are the corresponding normal laws. Standard normal and normal laws

[F2]

ϕ is a positive normalized Lebesgue density. The standard normal density has total mass one

[F4]

A bivariate additive-noise equation has the form Y=f(X)+N with independent X,N. Continuous additive-noise models on finite DAGs

[F5]

Condition 19 is inequality with its displayed differential equation at at least one point where ν′′(y−f(x))f′(x)≠0. Condition 19 and restricted additive-noise models

Verification

Given: The independent standard normal variables X,N and the definitions in the Example.

1.1givenA1F1F2F4

Under AC [A1], [F1]–[F2] and independence give the density ϕ(x)ϕ(n)=(2π)−1e−(x2+n2)/2 for (X,N). The forward equation Y=X+N is an additive-noise equation by [F4].

2.1step 1.1F3algebra

The linear map (x,n)↦(y,m)=(x+n,(x−n)/2) has determinant −1 and inverse (y,m)↦(x,n)=(y/2+m,y/2−m), whose determinant also has absolute value 1. By [F3], substituting the inverse into the density from step 1.1 gives pY,M(y,m)=12πexp⁡ ⁣(−(y/2+m)2+(y/2−m)22)=12πe−y2/4−m2.

3.1step 2.1F1F2algebra

The last density factors as pY(y)pM(m) with pY(y)=(2π)−1e−y2/4 and pM(m)=π−1/2e−m2. Each factor integrates to one by the affine normal-law description [F1] and normalization [F2], so the joint law is the product of its marginals and M⊥Y. Since M=X−Y/2, rearranging gives X=Y/2+M.

4.1givenF5algebra∎

For f(x)=x and standard normal input and noise, ξ(x)=ν(x)=−x2/2−12log⁡(2π), f′=1, f′′=f′′′=0, ξ′′′=ν′′′=0, and ν′′=−1. The Condition 19 domain is all (x,y) because ν′′(y−f(x))f′(x)=−1≠0; both sides of its equation equal zero there. Thus its required inequality never holds, so Condition 19 fails.

ExampleConstruction: AI-generatedVerification: AI-generatedOpen item page →

An identifiable nonlinear ANM with a cubic cause-to-effect function

Example

Assume AC. Let X,N be independent standard normal random variables and set Y=X3+N. The structural function is nonconstant and C3, and both noise densities are strictly positive and C3. For f(x)=x3 and standard normal input and noise, the triple satisfies Condition 19: at (x,y)=(1,0) its left side is 0 and its right side is 28. The bivariate direction-identifiability theorem therefore excludes every reverse additive-noise representation with an independent residual and a C3 structural function.

Facts & Assumptions

Given: Assume AC and take independent X,N∼N(0,1) with standard normal density ϕ(t)=(2π)−1/2e−t2/2.

[A1]

AC is the Axiom of Choice and implies countable choice (ACω), the additional axiom interface used by the standard-normal suppliers. The Axiom of Choice, The Axiom of Countable Choice (ACω), AC implies DC implies countable choice

[F1]

The standard normal law has density ϕ, and this density is positive and normalized. Standard normal and normal laws, The standard normal density has total mass one

[F2]

For a smooth bivariate ANM, Condition 19 fails when its displayed equation holds at every point of the nonzero domain. Condition 19 and restricted additive-noise models

[F3]

If Condition 19 holds, no reverse ANM in the stated smooth class represents the same observational law. Bivariate additive-noise direction identifiability under Condition 19

[F4]

The bivariate forward joint density is the product of the input density and shifted noise density. Positive joint density of a finite additive-noise model

Verification

Given: The independent standard normal variables X,N and Y=X3+N.

1.1givenA1F1F4construct

Under AC [A1], the equation is a bivariate additive-noise model with f(x)=x3, independent noise, strictly positive C3 input and noise densities, and nonconstant C3 function. By [F1] and [F4], its joint density is p(x,y)=ϕ(x)ϕ(y−x3).

1.2givenF1algebra

Put z=y−f(x). The standard normal log densities give ξ′′(x)=−1, ξ′′′(x)=0, ν′(z)=−z, ν′′(z)=−1, and ν′′′(z)=0. At (x,y)=(1,0), z=−1, f′=3, f′′=6, and f′′′=6, so ν′′(z)f′=−3≠0.

2.1F2F3step 1.2algebra

Substitution into Condition 19's right side gives (−1)(63)−2(−1)(6)(3)+(1)(6)+0−(1)623=−2+36+6−12=28, whereas ξ′′′(1)=0. Hence Condition 19 holds. The theorem [F3] now excludes a reverse ANM in its stated class, proving the Example's identifiability assertion.

3.1step 1.1step 1.2step 2.1∎

The input and noise densities, and the cubic function, satisfy the hypotheses in the Statement; the nonzero-domain witness in step 1.2 satisfies the Condition 19 inequality in step 2.1.

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