Wasserstein barycenters and applications in image processing: Difference between revisions
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==Introduction== | ==Introduction== | ||
===Motivation=== | ===Motivation=== | ||
Barycenters in physics and geometry are points that represent a notion of a [https://en.wikipedia.org/wiki/Mean mean] of a number of objects. In astronomy, the barycenter is the center of mass of two or more objects that orbit each other, and in geometry, a centroid is the [https://en.wikipedia.org/wiki/Arithmetic_mean arithmetic mean] of all the points in an object. Wasserstein barycenters attempt to capture this concept for probability measures. | Barycenters in physics and geometry are points that represent a notion of a [https://en.wikipedia.org/wiki/Mean mean] of a number of objects. In astronomy, the barycenter is the center of mass of two or more objects that orbit each other, and in geometry, a centroid is the [https://en.wikipedia.org/wiki/Arithmetic_mean arithmetic mean] of all the points in an object. Given countably many points <math>\{x_i\}_{i \in I}</math> in <math>R^n</math> with nonnegative weights <math>\{\lambda_i \}_{i \in I}</math>, the weighted <math>L^2</math> barycenter of the points is the unique point <math>y</math> minimizing <math>\sum_{i \in I} \lambda _i ||y - x_i||_2^2</math>. Wasserstein barycenters attempt to capture this concept for probability measures by replacing the [https://en.wikipedia.org/wiki/Euclidean_distance Euclidean distance] with the [https://en.wikipedia.org/wiki/Wasserstein_metric Wasserstein metric]. | ||
===Definition=== | ===Definition=== | ||
To generalize this to Wasserstein spaces, let <math>\Omega</math> be a domain and <math>P(\Omega)</math> be the set of probability measures on <math>\Omega</math>. Given a collection of probability measures <math> \{\mu_i / \rho_i \}_{i \in I}</math> and nonnegative weights <math>\{\lambda_i\}_{i \in I}</math>, we define a weighted barycenter of <math>\{\mu\}</math> as any probability measure <math>\mu/\rho</math> that minimizes | |||
<math>\sum_{i \in I} \lambda_i W_2^2( \rho_i, \rho)^2</math> | <math>\sum_{i \in I} \lambda_i W_2^2( \rho_i, \rho)^2</math> | ||
over the space <math>\rho \in P(\Omega)</math>. | over the space <math>\rho \in P(\Omega)</math>. |
Revision as of 20:58, 11 February 2022
In optimal transport, a Wasserstein barycenter (Insert reference of Sant) is a probability measure that acts as a center of mass between two or more probability measures. It generalizes the notions of physical barycenters and geometric centroids.
Introduction
Motivation
Barycenters in physics and geometry are points that represent a notion of a mean of a number of objects. In astronomy, the barycenter is the center of mass of two or more objects that orbit each other, and in geometry, a centroid is the arithmetic mean of all the points in an object. Given countably many points in with nonnegative weights , the weighted barycenter of the points is the unique point minimizing . Wasserstein barycenters attempt to capture this concept for probability measures by replacing the Euclidean distance with the Wasserstein metric.
Definition
To generalize this to Wasserstein spaces, let be a domain and be the set of probability measures on . Given a collection of probability measures and nonnegative weights , we define a weighted barycenter of as any probability measure that minimizes over the space .
Existence and Uniqueness
Other spaces
Applications
Barycenters in Image processing
Generalizations
Wasserstein barycenters are examples of Karcher and Fr%C3%A9chet means where the distance function used is the Wasserstein distance.