English

Conditional Hardness of Earth Mover Distance

Computational Complexity 2019-09-25 v1

Abstract

The Earth Mover Distance (EMD) between two sets of points A,BRdA, B \subseteq \mathbb{R}^d with A=B|A| = |B| is the minimum total Euclidean distance of any perfect matching between AA and BB. One of its generalizations is asymmetric EMD, which is the minimum total Euclidean distance of any matching of size A|A| between sets of points A,BRdA,B \subseteq \mathbb{R}^d with AB|A| \leq |B|. The problems of computing EMD and asymmetric EMD are well-studied and have many applications in computer science, some of which also ask for the EMD-optimal matching itself. Unfortunately, all known algorithms require at least quadratic time to compute EMD exactly. Approximation algorithms with nearly linear time complexity in nn are known (even for finding approximately optimal matchings), but suffer from exponential dependence on the dimension. In this paper we show that significant improvements in exact and approximate algorithms for EMD would contradict conjectures in fine-grained complexity. In particular, we prove the following results: (1) Under the Orthogonal Vectors Conjecture, there is some c>0c>0 such that EMD in Ω(clogn)\Omega(c^{\log^* n}) dimensions cannot be computed in truly subquadratic time. (2) Under the Hitting Set Conjecture, for every δ>0\delta>0, no truly subquadratic time algorithm can find a (1+1/nδ)(1 + 1/n^\delta)-approximate EMD matching in ω(logn)\omega(\log n) dimensions. (3) Under the Hitting Set Conjecture, for every η=1/ω(logn)\eta = 1/\omega(\log n), no truly subquadratic time algorithm can find a (1+η)(1 + \eta)-approximate asymmetric EMD matching in ω(logn)\omega(\log n) dimensions.

Keywords

Cite

@article{arxiv.1909.11068,
  title  = {Conditional Hardness of Earth Mover Distance},
  author = {Dhruv Rohatgi},
  journal= {arXiv preprint arXiv:1909.11068},
  year   = {2019}
}

Comments

15 pages, 1 figure

R2 v1 2026-06-23T11:24:37.986Z