Geodesics and generalized geodesics

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Introduction

There are many ways that we can describe Wasserstein metric. One of them is to characterize absolutely continuos curves (AC)(p.188[1]) and provide a dynamic formulation of the special case Namely, it is possible to see as an infimum of the lengts of curves that satisfy Continuity equation
().

Geodesics in general metric spaces

First, we will introduce definition of the geodesic in general metric space . We are going to follow presentation from the book by Santambrogio[1].

Definition. A curve is said to be geodesic in if it minimizes the length of all the curves
such that and .

Since we have a definition of a geodesic in the general space, it is natural to think of Riemannian structure. It can be defined. More about this topic can be seen in the following article Formal Riemannian Structure of the Wasserstein_metric.

Now, we proceed with necessary definitions in order to be able to understand Wasserstein metric in a different way.

Definition. A metric space is called a length space if it holds
                    
Definition. In a length space, a curve is said to be constant speed geodesic between and in if it satisfies
                     for all 

It is clear that constant speed geodesic curve is geodesic curve.

Statement of Theorem

Now, we can rephrase Wasserstein metrics in dynamic language. In special case, for :

Theorem.(Benamou-Brenier)[1] Let . Then we have
      

Generalization

It is possible to generalize the previous theorem and theory to metrics. More about that could be seen in the book [2].

However, it is possible to generalize theorem for a different kind of geodesics [3].

References