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The Chain Rule for Free Difference Quotients under an Affine Substitution

Free difference quotients transform under an affine substitution through the transpose of its linear part, as in the classical chain rule.

Statement

In the setting of Noncommutative Laws, Couplings and the Wasserstein Distance: Standing Notation, let m,n∈Nm,n\in\mathbb{N}, let T=(A,c)T=(A,c) be an affine datum from mm to nn variables with affine substitution σT:Pn→Pm\sigma_{T}:\mathcal{P}_{n}\to\mathcal{P}_{m}, let γ∈Σm\gamma\in\Sigma_{m}, and let μ=γ∘σT\mu=\gamma\circ\sigma_{T}, which belongs to Σn\Sigma_{n} by Affine Substitutions of Noncommutative Laws: Self-Adjointness, Composition, Moment Formulas and Positivity, and the Coordinate Data §self-adjoint. Let ∂kγ\partial^{\gamma}_{k} and ∂iμ\partial^{\mu}_{i} be the free difference quotients of γ\gamma and μ\mu.

For every p∈Pnp\in\mathcal{P}_{n} and every k∈[m]k\in[m],

∂kγ(σT(p))=∑i=1nAik ∂iμ(p).\partial^{\gamma}_{k}\bigl(\sigma_{T}(p)\bigr)=\sum_{i=1}^{n}A_{ik}\,\partial^{\mu}_{i}(p).

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