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For a proper convex function $\Phi$ and its convex conjugate ${\Phi }^{\ast }$, this gap is nonnegative by the Fenchel–Young inequality. It vanishes exactly when $y\in \partial \Phi (x)$. Its integral against a transport plan is the difference between the half-squared-distance cost and the value of the integrable Kantorovich potentials $u=|x{|}^2/2-\Phi$, $v=|y{|}^2/2-{\Phi }^{\ast }$.

For probability measures on ${\mathbb{R}}^d$ with finite second moments, a transport plan minimizes the quadratic cost exactly when it is concentrated on the graph of the subdifferential of a sequentially lower semicontinuous proper convex function.

For probability measures $\mu ,\nu$ on ${\mathbb{R}}^d$ with finite second moments, the Knott–Smith optimality criterion states that a transport plan $\pi \in \Pi (\mu ,\nu )$ minimizes the quadratic cost $|x-y{|}^2$ if and only if there is a proper convex function $\Phi :{\mathbb{R}}^d\to \mathbb{R}\cup \{+\infty \}$ that is sequentially lower semicontinuous and satisfiesThe subdifferential is characterized bywith $\Phi (x)<\infty$. Thus the transport plan is concentrated on the graph of the subdifferential. No absolute continuity of measures assumption on $\mu$ is needed. Multiplying the cost by $1/2$ leaves the criterion unchanged. The original quadratic optimal mapping result is Knott and Smith, On the optimal mapping of distributions.

A standard sufficient form of Brenier theorem assumes $\mu ,\nu \in \mathcal{P}({\mathbb{R}}^d)$ have finite second moments and $\mu \ll {\mathcal{L}}^d$, that is, absolute continuity of measures with respect to Lebesgue measure. For the cost $|x-y{|}^2$, there exists a unique optimal transport plan, and it is induced by a transport map:Here $\Phi$ is a proper convex function, which may be chosen sequentially lower semicontinuous, and its gradient exists $\mu$-almost everywhere. The map $\nabla \Phi$ is unique $\mu$-almost everywhere and is the unique minimizer of the Monge optimal transport problem; its cost equals the Kantorovich optimal transport problem minimum. Equivalently, it is the unique gradient of a convex function transporting $\mu$ to $\nu$.

The uniqueness claim concerns the map and the transport plan, not a globally unique potential. The potential may be shifted by a constant, and additional nonuniqueness away from the source can occur. No density assumption is required on $\nu$. A primary reference is Brenier's Polar factorization and monotone rearrangement of vector-valued functions.

An extended-real function is proper if it never takes $-\infty$ and is finite at at least one point. It can take $+\infty$ to impose a constraint. A convex function with this property is a proper convex function.