Wasserstein metric

In mathematics, the Wasserstein distance or Kantorovich– metric is a distance function defined between probability distributions on a given metric space ${\displaystyle M}$.

Intuitively, if each distribution is viewed as a unit amount of earth (soil) piled on ${\displaystyle M}$, the metric is the minimum "cost" of turning one pile into the other, which is assumed to be the amount of earth that needs to be moved times the mean distance it has to be moved. Because of this analogy, the metric is known in computer science as the earth mover's distance.

The name "Wasserstein distance" was coined by R. L. Dobrushin in 1970, after learning of it in the work of Russian mathematician Leonid Vaseršteĭn 1969, however the metric was first defined by Leonid Kantorovich in The Mathematical Method of Production Planning and Organization (Russian original 1939) in the context of optimal transport planning of goods and materials. Some scholars thus encourage use of the terms "Kantorovich metric" and "Kantorovich distance". Most English-language publications use the German spelling "Wasserstein" (attributed to the name "Vaseršteĭn" being of German origin).

Definition[]

Let ${\displaystyle (M,d)}$ be a metric space for which every Borel probability measure on ${\displaystyle M}$ is a Radon measure (a so-called Radon space). For ${\displaystyle p\geq 1}$, let ${\displaystyle P_{p}(M)}$ denote the collection of all probability measures ${\displaystyle \mu }$ on ${\displaystyle M}$ with finite ${\displaystyle p^{\text{th}}}$ moment. Then, there exists some ${\displaystyle x_{0}}$ in ${\displaystyle M}$ such that:

${\displaystyle \int _{M}d(x,x_{0})^{p}\,\mathrm {d} \mu (x)<\infty .}$

The ${\displaystyle p^{\text{th}}}$ Wasserstein distance between two probability measures ${\displaystyle \mu }$ and ${\displaystyle \nu }$ in ${\displaystyle P_{p}(M)}$ is defined as

${\displaystyle W_{p}(\mu ,\nu ):=\left(\inf _{\gamma \in \Gamma (\mu ,\nu )}\int _{M\times M}d(x,y)^{p}\,\mathrm {d} \gamma (x,y)\right)^{1/p},}$

where ${\displaystyle \Gamma (\mu ,\nu )}$ denotes the collection of all measures on ${\displaystyle M\times M}$ with marginals ${\displaystyle \mu }$ and ${\displaystyle \nu }$ on the first and second factors respectively. (The set ${\displaystyle \Gamma (\mu ,\nu )}$ is also called the set of all couplings of ${\displaystyle \mu }$ and ${\displaystyle \nu }$.)

The above distance is usually denoted ${\displaystyle W_{p}(\mu ,\nu )}$ (typically among authors who prefer the "Wasserstein" spelling) or ${\displaystyle \ell _{p}(\mu ,\nu )}$ (typically among authors who prefer the "Vaserstein" spelling). The remainder of this article will use the ${\displaystyle W_{p}}$ notation.

The Wasserstein metric may be equivalently defined by

${\displaystyle W_{p}(\mu ,\nu )=\left(\inf \operatorname {E} {\big [}d(X,Y)^{p}{\big ]}\right)^{1/p},}$

where ${\displaystyle \mathbf {E} [Z]}$ denotes the expected value of a random variable ${\displaystyle Z}$ and the infimum is taken over all joint distributions of the random variables ${\displaystyle X}$ and ${\displaystyle Y}$ with marginals ${\displaystyle \mu }$ and ${\displaystyle \nu }$ respectively.

Intuition and connection to optimal transport[]

Two one-dimensional distributions ${\displaystyle \mu }$ and ${\displaystyle \nu }$, plotted on the x and y axes, and one possible joint distribution that defines a transport plan between them. The joint distribution/transport plan is not unique

One way to understand the above definition is to consider the optimal transport problem. That is, for a distribution of mass ${\displaystyle \mu (x)}$ on a space ${\displaystyle X}$, we wish to transport the mass in such a way that it is transformed into the distribution ${\displaystyle \nu (x)}$ on the same space; transforming the 'pile of earth' ${\displaystyle \mu }$ to the pile ${\displaystyle \nu }$. This problem only makes sense if the pile to be created has the same mass as the pile to be moved; therefore without loss of generality assume that ${\displaystyle \mu }$ and ${\displaystyle \nu }$ are probability distributions containing a total mass of 1. Assume also that there is given some cost function

${\displaystyle c(x,y)\mapsto [0,\infty )}$

that gives the cost of transporting a unit mass from the point ${\displaystyle x}$ to the point ${\displaystyle y}$. A transport plan to move ${\displaystyle \mu }$ into ${\displaystyle \nu }$ can be described by a function ${\displaystyle \gamma (x,y)}$ which gives the amount of mass to move from ${\displaystyle x}$ to ${\displaystyle y}$. You can imagine the task as the need to move a pile of earth of shape ${\displaystyle \mu }$ to the hole in the ground of shape ${\displaystyle \nu }$ such that at the end, both the pile of earth and the hole in the ground completely vanish. In order for this plan to be meaningful, it must satisfy the following properties

${\displaystyle {\begin{aligned}\int \gamma (x,y)\,\mathrm {d} y=\mu (x)&\qquad {\text{(the amount of earth moved out of point }}x{\text{ needs to equal the amount that was there to begin with)}}\\\int \gamma (x,y)\,\mathrm {d} x=\nu (y)&\qquad {\text{(the amount of earth moved into point }}y{\text{ needs to equal the depth of the hole that was there at the beginning)}}\end{aligned}}}$

That is, that the total mass moved out of an infinitesimal region around ${\displaystyle x}$ must be equal to ${\displaystyle \mu (x)\mathrm {d} x}$ and the total mass moved into a region around ${\displaystyle y}$ must be ${\displaystyle \nu (y)\mathrm {d} y}$. This is equivalent to the requirement that ${\displaystyle \gamma }$ be a joint probability distribution with marginals ${\displaystyle \mu }$ and ${\displaystyle \nu }$. Thus, the infinitesimal mass transported from ${\displaystyle x}$ to ${\displaystyle y}$ is ${\displaystyle \gamma (x,y)\,\mathrm {d} x\,\mathrm {d} y}$, and the cost of moving is ${\displaystyle c(x,y)\gamma (x,y)\,\mathrm {d} x\,\mathrm {d} y}$, following the definition of the cost function. Therefore, the total cost of a transport plan ${\displaystyle \gamma }$ is

${\displaystyle \iint c(x,y)\gamma (x,y)\,\mathrm {d} x\,\mathrm {d} y=\int c(x,y)\,\mathrm {d} \gamma (x,y)}$

The plan ${\displaystyle \gamma }$ is not unique; the optimal transport plan is the plan with the minimal cost out of all possible transport plans. As mentioned, the requirement for a plan to be valid is that it is a joint distribution with marginals ${\displaystyle \mu }$ and ${\displaystyle \nu }$; letting ${\displaystyle \Gamma }$ denote the set of all such measures as in the first section, the cost of the optimal plan is

${\displaystyle C=\inf _{\gamma \in \Gamma (\mu ,\nu )}\int c(x,y)\,\mathrm {d} \gamma (x,y)}$

If the cost of a move is simply the distance between the two points, then the optimal cost is identical to the definition of the ${\displaystyle W_{1}}$ distance.

Examples[]

Point masses (degenerate distributions)[]

Let ${\displaystyle \mu _{1}=\delta _{a_{1}}}$ and ${\displaystyle \mu _{2}=\delta _{a_{2}}}$ be two degenerate distributions (i.e. Dirac delta distributions) located at points ${\displaystyle a_{1}}$ and ${\displaystyle a_{2}}$ in ${\displaystyle \mathbb {R} }$. There is only one possible coupling of these two measures, namely the point mass ${\displaystyle \delta _{(a_{1},a_{2})}}$ located at ${\displaystyle (a_{1},a_{2})\in \mathbb {R} ^{2}}$. Thus, using the usual absolute value function as the distance function on ${\displaystyle \mathbb {R} }$, for any ${\displaystyle p\geq 1}$, the ${\displaystyle p}$-Wasserstein distance between ${\displaystyle \mu _{1}}$ and ${\displaystyle \mu _{2}}$ is

${\displaystyle W_{p}(\mu _{1},\mu _{2})=|a_{1}-a_{2}|.}$

By similar reasoning, if ${\displaystyle \mu _{1}=\delta _{a_{1}}}$ and ${\displaystyle \mu _{2}=\delta _{a_{2}}}$ are point masses located at points ${\displaystyle a_{1}}$ and ${\displaystyle a_{2}}$ in ${\displaystyle \mathbb {R} ^{n}}$, and we use the usual Euclidean norm on ${\displaystyle \mathbb {R} ^{n}}$ as the distance function, then

${\displaystyle W_{p}(\mu _{1},\mu _{2})=\|a_{1}-a_{2}\|_{2}.}$

Normal distributions[]

Let ${\displaystyle \mu _{1}={\mathcal {N}}(m_{1},C_{1})}$ and ${\displaystyle \mu _{2}={\mathcal {N}}(m_{2},C_{2})}$ be two non-degenerate Gaussian measures (i.e. normal distributions) on ${\displaystyle \mathbb {R} ^{n}}$, with respective expected values ${\displaystyle m_{1}}$ and ${\displaystyle m_{2}\in \mathbb {R} ^{n}}$ and symmetric positive semi-definite covariance matrices ${\displaystyle C_{1}}$ and ${\displaystyle C_{2}\in \mathbb {R} ^{n\times n}}$. Then,^[1] with respect to the usual Euclidean norm on ${\displaystyle \mathbb {R} ^{n}}$, the 2-Wasserstein distance between ${\displaystyle \mu _{1}}$ and ${\displaystyle \mu _{2}}$ is

${\displaystyle W_{2}(\mu _{1},\mu _{2})^{2}=\|m_{1}-m_{2}\|_{2}^{2}+\mathop {\mathrm {trace} } {\bigl (}C_{1}+C_{2}-2{\bigl (}C_{2}^{1/2}C_{1}C_{2}^{1/2}{\bigr )}^{1/2}{\bigr )}.}$

This result generalises the earlier example of the Wasserstein distance between two point masses (at least in the case ${\displaystyle p=2}$), since a point mass can be regarded as a normal distribution with covariance matrix equal to zero, in which case the trace term disappears and only the term involving the Euclidean distance between the means remains.

Applications[]

The Wasserstein metric is a natural way to compare the probability distributions of two variables X and Y, where one variable is derived from the other by small, non-uniform perturbations (random or deterministic).

In computer science, for example, the metric W₁ is widely used to compare discrete distributions, e.g. the color histograms of two digital images; see earth mover's distance for more details.

In their paper 'Wasserstein GAN', Arjovsky et al.^[2] use the Wasserstein-1 metric as a way to improve the original framework of Generative Adversarial Networks (GAN), to alleviate the vanishing gradient and the mode collapse issues. The special case of normal distributions is used in a Frechet Inception Distance.

The Wasserstein metric has a formal link with Procrustes analysis, with application to chirality measures,^[3] and to shape analysis.^[4]

Properties[]

Metric structure[]

It can be shown that W_p satisfies all the axioms of a metric on P_p(M). Furthermore, convergence with respect to W_p is equivalent to the usual weak convergence of measures plus convergence of the first pth moments.^[5]

Dual representation of W₁[]

The following dual representation of W₁ is a special case of the duality theorem of Kantorovich and Rubinstein (1958): when μ and ν have bounded support,

${\displaystyle W_{1}(\mu ,\nu )=\sup \left\{\left.\int _{M}f(x)\,\mathrm {d} (\mu -\nu )(x)\right|{\text{continuous }}f:M\to \mathbb {R} ,\operatorname {Lip} (f)\leq 1\right\},}$

where Lip(f) denotes the minimal Lipschitz constant for f.

Compare this with the definition of the Radon metric:

${\displaystyle \rho (\mu ,\nu ):=\sup \left\{\left.\int _{M}f(x)\,\mathrm {d} (\mu -\nu )(x)\right|{\text{continuous }}f:M\to [-1,1]\right\}.}$

If the metric d is bounded by some constant C, then

${\displaystyle 2W_{1}(\mu ,\nu )\leq C\rho (\mu ,\nu ),}$

and so convergence in the Radon metric (identical to total variation convergence when M is a Polish space) implies convergence in the Wasserstein metric, but not vice versa.

Equivalence of W₂ and a negative-order Sobolev norm[]

Under suitable assumptions, the Wasserstein distance ${\displaystyle W_{2}}$ of order two is Lipschitz equivalent to a negative-order homogeneous Sobolev norm.^[6] More precisely, if we take ${\displaystyle M}$ to be a connected Riemannian manifold equipped with a positive measure ${\displaystyle \pi }$, then we may define for ${\displaystyle f\colon M\to \mathbb {R} }$ the seminorm

${\displaystyle \|f\|_{{\dot {H}}^{1}(\pi )}^{2}=\int _{M}|\nabla f(x)|^{2}\,\pi (\mathrm {d} x)}$

and for a signed measure ${\displaystyle \mu }$ on ${\displaystyle M}$ the dual norm

${\displaystyle \|\mu \|_{{\dot {H}}^{-1}(\pi )}=\sup {\bigg \{}|\langle f,\mu \rangle |\,{\bigg |}\,\|f\|_{{\dot {H}}^{1}(\pi )}\leq 1{\bigg \}}.}$

Then any two probability measures ${\displaystyle \mu }$ and ${\displaystyle \nu }$ on ${\displaystyle M}$ satisfy the upper bound

${\displaystyle W_{2}(\mu ,\nu )\leq 2\|\mu -\nu \|_{{\dot {H}}^{-1}(\mu )}.}$

In the other direction, if ${\displaystyle \mu }$ and ${\displaystyle \nu }$ each have densities with respect to the standard volume measure on ${\displaystyle M}$ that are both bounded above some ${\displaystyle 0<C<\infty }$, and ${\displaystyle M}$ has non-negative Ricci curvature, then

${\displaystyle \|\mu -\nu \|_{{\dot {H}}^{-1}(\mu )}\leq {\sqrt {C}}W_{2}(\mu ,\nu ).}$

Separability and completeness[]

For any p ≥ 1, the metric space (P_p(M), W_p) is separable, and is complete if (M, d) is separable and complete.^[7]

See also[]

• Lévy metric
• Lévy–Prokhorov metric
• Total variation distance of probability measures
• Transportation theory
• Earth mover's distance

This article includes a list of general references, but it remains largely unverified because it lacks sufficient corresponding inline citations. Please help to improve this article by introducing more precise citations. (July 2012) (Learn how and when to remove this template message)

References[]

• Villani, Cédric (2008). Optimal Transport, Old and New. Springer. ISBN 978-3-540-71050-9.
• Ambrosio, L., Gigli, N. & Savaré, G. (2005). Gradient Flows in Metric Spaces and in the Space of Probability Measures. Basel: ETH Zürich, Birkhäuser Verlag. ISBN 3-7643-2428-7.CS1 maint: multiple names: authors list (link)
• Jordan, Richard; Kinderlehrer, David; Otto, Felix (1998). "The variational formulation of the Fokker–Planck equation". SIAM J. Math. Anal. 29 (1): 1–17 (electronic). CiteSeerX 10.1.1.6.8815. doi:10.1137/S0036141096303359. ISSN 0036-1410. MR 1617171.
• Rüschendorf, L. (2001) [1994], "Wasserstein metric", Encyclopedia of Mathematics, EMS Press

External links[]

• "What is the advantages of Wasserstein metric compared to Kullback–Leibler divergence?". Stack Exchange. August 1, 2017.