2013
DOI: 10.1007/s00526-013-0657-x
|View full text |Cite
|
Sign up to set email alerts
|

Non-branching geodesics and optimal maps in strong $$CD(K,\infty )$$ C D ( K , ∞ ) -spaces

Abstract: We prove that in metric measure spaces where the entropy functional is Kconvex along every Wasserstein geodesic any optimal transport between two absolutely continuous measures with finite second moments lives on a non-branching set of geodesics. As a corollary we obtain that in these spaces there exists only one optimal transport plan between any two absolutely continuous measures with finite second moments and this plan is given by a map.The results are applicable in metric measure spaces having Riemannian R… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
121
0

Year Published

2014
2014
2024
2024

Publication Types

Select...
9

Relationship

1
8

Authors

Journals

citations
Cited by 105 publications
(122 citation statements)
references
References 20 publications
1
121
0
Order By: Relevance
“…In the paper we will only consider essentially non-branching spaces, let us recall their definition (introduced in [46]).…”
Section: Backgroundsmentioning
confidence: 99%
“…In the paper we will only consider essentially non-branching spaces, let us recall their definition (introduced in [46]).…”
Section: Backgroundsmentioning
confidence: 99%
“…Recall that an mms is essentially non-branching and satisfies the (CD-)CD * -condition if and only if it satisfies the strong (CD-)CD * -condition; for these results and definitions see [5,30]. The CD-, CD * -, and MCP-conditions allow for non-Riemannian geometries which include, but are not restricted to, Finsler manifolds.…”
Section: Moreover If Iso(x) Is a Lie Group Then Iso M (X) Is So As Wellmentioning
confidence: 99%
“…More precisely, since each condition implies CD(K, ∞), together with infinitesimally Hilbertianness (X, d, m) satisfies the condition RCD(K, ∞) in the sense of [AGS14b]. Therefore, the Boltzmann-Shanon entropy is even strongly K-convex, and hence (X, d, m) is essentially non-branchning by [RS14]. Then, first we know that CD * (K, N ) is equivalent to CD e (K, N ) by [EKS15].…”
Section: 2mentioning
confidence: 99%