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A REMARK ON THE GEOMETRIC INTERPRETATION OF THE A3W CONDITION FROM OPTIMAL TRANSPORT

Published online by Cambridge University Press:  13 October 2022

CALE RANKIN*
Affiliation:
Fields Institute for Research in Mathematical Sciences, Toronto, ON M5T 3J1, Canada
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Abstract

We provide a geometric interpretation of the well-known A3w condition for regularity in optimal transport.

Type
Research Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
Copyright
© The Author(s), 2022. Published by Cambridge University Press on behalf of Australian Mathematical Publishing Association Inc.

1 Introduction

In optimal transport, a condition known as A3w is necessary for regularity of the optimal transport map. Here we provide a geometric interpretation of A3w. We use freely the notation from [Reference Ma, Trudinger and Wang4]. Let $c \in C^2(\mathbf {R}^n \times \mathbf {R}^n)$ satisfy A1 and A2 (see Section 2). Keeping in mind the prototypical case $c(x,y) = |x-y|^2$ , we fix $x_0,y_0 \in \mathbf {R}^n$ and perform a linear transformation so that $c_{xy}(x_0,y_0) = -I$ . Define coordinates

(1.1) $$ \begin{align} q(x)&:= -c_y(x,y_0), \end{align} $$
(1.2) $$ \begin{align} p(\,y)&:= -c_x(x_0,y), \end{align} $$

and denote the inverse transformations by $x(q),y(p)$ . Write $c(q,p) = c(x(q),y(p))$ and let $q_0=q(x_0)$ and $p_0=p(\,y_0)$ . We prove A3w is satisfied if and only if whenever these transformations are performed,

$$ \begin{align*} (q-q_0)\cdot (p-p_0) \geq 0 {\implies} c(q,p)+c(q_0,p_0) \leq c(q,p_0)+c(q_0,p). \end{align*} $$

Heuristically, A3w implies that when $q-q_0$ ‘points in the same direction’ as $p-p_0$ , it is cheaper to transport q to p and $q_0$ to $p_0$ than the alternative q to $p_0$ and $q_0$ to p. Thus, A3w represents compatibility between directions in the cost-convex geometry and the cost of transport.

A3w first appeared (in a stronger form) in [Reference Ma, Trudinger and Wang4]. It was weakened in [Reference Trudinger and Wang6] and a new interpretation was given in [Reference Loeper2]. The impetus for the above interpretation is Lemma 2.1 in [Reference Chen and Wang1]. Our result can also be realised by a particular choice of c-convex function in the unpublished preprint [Reference Trudinger and Wang5].

2 Proof of result

Let $c \in C^2(\mathbf {R}^n \times \mathbf {R}^n)$ satisfy the following well-known conditions.

  1. A1. For each $x_0,y_0 \in \mathbf {R}^n$ , the mappings

    $$ \begin{align*} x \mapsto c_y(x,y_0) \quad\text{and} \quad y \mapsto c_x(x_0,y) \end{align*} $$
    are injective.
  2. A2. For each $x_0,y_0 \in \mathbf {R}^n$ , we have $\det c_{i,j}(x_0,y_0) \neq 0$ .

Here, and throughout, subscripts before a comma denote differentiation with respect to the first variable, subscripts after a comma denote differentiation with respect to the second variable.

By A1, we define on $\mathcal {U}:= \{(x,c_x(x,y)): x,y \in \mathbf {R}^n\}$ a mapping $Y:\mathcal {U}\rightarrow \mathbf {R}^n$ by

$$ \begin{align*} c_x(x,Y(x,p)) = p. \end{align*} $$

The A3w condition, usually expressed with fourth derivatives but written here as in [Reference Loeper and Trudinger3], is the following statement.

  1. A3w. Fix x. The function

    $$ \begin{align*} p \mapsto c_{ij}(x,Y(x,p))\xi_i\xi_j\end{align*} $$
    is concave along line segments orthogonal to $\xi $ .

To verify A3w, it suffices to verify the midpoint concavity, that is, whenever ${\xi \cdot \eta = 0}$ , it follows that

(2.1) $$ \begin{align} 0 \geq [c_{ij}(x,Y(x,p+\eta)) - 2c_{ij}(x,Y(x,p)) + c_{ij}(x,Y(x,p-\eta))]\xi_i\xi_j. \end{align} $$

Finally, we recall that a set $A \subset \mathbf {R}^n$ is called c-convex with respect to $y_0$ provided $c_y(A,y_0)$ is convex. When the A3w condition is satisfied and $y,y_0 \in \mathbf {R}^n$ are given, the section $\{x \in \mathbf {R}^n: c(x,y)> c(x,y_0)\}$ is c-convex with respect to $y_0$ [Reference Loeper and Trudinger3].

Now fix $(x_0,p_0) \in \mathcal {U}$ and $y_0 = Y(x_0,p_0)$ . To simplify the proof, we assume $x_0,y_0,q_0,p_0 = 0$ . Up to an affine transformation (replace y with $\tilde {y}:=-c_{xy}(0,0)y$ ), we assume $c_{xy}(0,0) = -I$ . Note that with $q,p$ , as defined in (1.1), (1.2), this implies ${\partial q}/{\partial x}(0) = I$ . Put

$$ \begin{align*} \tilde{c}(x,y) &:= c(x,y) - c(x,0) - c(0,y) + c(0,0),\\ \overline{c}(q,p) &:= \tilde{c}(x(q),y(p)). \end{align*} $$

Theorem 2.1. The A3w condition is satisfied if and only if whenever the above transformations are applied, the following implication holds:

(2.2) $$ \begin{align} q \cdot p \geq 0 {\implies} \overline{c}(q,p) \leq 0. \end{align} $$

Proof. Observe by a Taylor series

(2.3) $$ \begin{align} \overline{c}(q,p) = -(q \cdot p) + \overline{c}_{ij}(\tau q,p)q_iq_j \end{align} $$

for some $\tau \in (0,1)$ . First, assume A3w and let $q \cdot p> 0$ . By (2.3), we have $\overline {c}(-tq,p)> 0 > \overline {c}(tq,p)$ for $t>0$ sufficiently small. If $\overline {c}(q,p)> 0$ , then the c-convexity (in our coordinates, convexity) of the section

$$ \begin{align*} \{ q : \overline{c}(q,p)> \overline{c}(q,0) = 0 \} \end{align*} $$

is violated. By continuity, $\overline {c}(q,p) \leq 0$ whenever $q \cdot p \geq 0$ .

In the other direction, take nonzero q with $q \cdot p = 0$ and small t. By (2.2) and (2.3),

$$ \begin{align*} 0 \geq \overline{c}(t q,p)/t^2 = \overline{c}_{ij}(t \tau q,p)q_iq_j. \end{align*} $$

This inequality also holds with $-p$ . Moreover, $\overline {c}_{ij}(t \tau q, 0) = 0$ . Thus,

$$ \begin{align*} 0 \geq [\overline{c}_{ij}(t \tau q,p) - 2\overline{c}_{ij}(t \tau q , 0) + \overline{c}_{ij}(t \tau q, -p)]q_iq_j.\end{align*} $$

Sending $t \rightarrow 0$ and returning to our original coordinates, we obtain (2.1).

Remark 2.2. On a Riemannian manifold with $c(x,y) = d(x,y)^2$ , for d the distance function, Loeper [Reference Loeper2] proved A3w implies nonnegative sectional curvature. Our result expedites his proof. Let $x_0=y_0 \in M$ and $u,v \in T_{x_0}M$ satisfy $u\cdot v = 0$ with $x = \exp _{x_0}(tu)$ and $y=\exp _{x_0}(tv)$ . Working in a sufficiently small local coordinate chart, our previous proof implies that if A3w is satisfied,

(2.4) $$ \begin{align} d(x,y)^2 \leq d(x_0,y)^2+d(x_0,x)^2 = 2t. \end{align} $$

The sectional curvature in the plane generated by $u,v$ is the $\kappa $ satisfying

(2.5) $$ \begin{align} d(\exp_{x_0}(tu),\exp_{x_0}(tv)) = \sqrt{2}t\bigg(1-\frac{\kappa}{12}t^2+O(t^3)\bigg) \quad\text{as }t \rightarrow 0, \end{align} $$

whereby comparison with (2.4) proves the result. (See [Reference Villani7, Equation (1)] for (2.5).) We note Loeper proved his result using an infinitesimal version of (2.4).

Acknowledgements

My thanks to Jiakun Liu and Robert McCann for helpful comments and discussion.

Footnotes

This research is supported by ARC DP 200101084 and the Fields Institute for Research in Mathematical Sciences.

References

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