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An identifiable nonlinear ANM with a cubic cause-to-effect function
Example
Assume AC. Let be independent standard normal random variables and set . The structural function is nonconstant and , and both noise densities are strictly positive and . For and standard normal input and noise, the triple satisfies Condition 19: at its left side is and its right side is . The bivariate direction-identifiability theorem therefore excludes every reverse additive-noise representation with an independent residual and a structural function.
Example references
The bivariate additive-noise equation and causal minimality
The Condition 19 equation and its nonzero domain
The bivariate identifiability conclusion under Condition 19
The positive forward joint density
Peters et al., JMLR (2014), Condition 19 and Theorem 20
Peters, Janzing, and Schölkopf, Elements of Causal Inference, §4.1.4, Theorem 4.5
Assaad, Devijver, and Gaussier, course notes (2023), slides 22–23
Facts & Assumptions
Given: Assume AC and take independent with standard normal density .
AC is the Axiom of Choice and implies countable choice (AC), the additional axiom interface used by the standard-normal suppliers. The Axiom of Choice, The Axiom of Countable Choice (), AC implies DC implies countable choice
The standard normal law has density , and this density is positive and normalized. Standard normal and normal laws, The standard normal density has total mass one
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
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
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 and .
Under AC [A1], the equation is a bivariate additive-noise model with , independent noise, strictly positive input and noise densities, and nonconstant function. By [F1] and [F4], its joint density is .
Put . The standard normal log densities give , , , , and . At , , , , and , so .
Substitution into Condition 19's right side gives whereas . Hence Condition 19 holds. The theorem [F3] now excludes a reverse ANM in its stated class, proving the Example's identifiability assertion.
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.
Depends on
- Continuous additive-noise models on finite DAGs
- Condition 19 and restricted additive-noise models
- Bivariate additive-noise direction identifiability under Condition 19
- Positive joint density of a finite additive-noise model
- The Axiom of Choice
- The Axiom of Countable Choice ($\mathrm{AC}_\omega$)
- AC implies DC implies countable choice
- Standard normal and normal laws
- The standard normal density has total mass one
Used by
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Sources
- Jonas Peters, Joris Mooij, Dominik Janzing, and Bernhard Schölkopf, Causal Discovery with Continuous Additive Noise Models, Condition 19 and Theorem 20 (standard reference, not scraped)
- Jonas Peters, Dominik Janzing, and Bernhard Schölkopf, Elements of Causal Inference, §4.1.4, Theorem 4.5 (standard reference, not scraped)
- K. Assaad, E. Devijver, and G. Gaussier, Causal discovery: noise-based methods, ENS Lyon course notes (2023), slides 22–23 (standard reference, not scraped)