English

Optimal Ballistic Transport and Hopf-Lax Formulae on Wasserstein Space

Analysis of PDEs 2017-06-13 v2

Abstract

We investigate the optimal mass transport problem associated to the following "ballistic" cost functional on phase space M×MM\times M^*, bT(v,x):=inf{v,γ(0)+0TL(γ(t),γ˙(t))dt,γC1([0,T),M),γ(T)=x}, b_T(v, x):=\inf\{\langle v, \gamma (0)\rangle +\int_0^TL(\gamma (t), {\dot \gamma}(t))\, dt, \gamma \in C^1([0, T), M), \gamma(T)=x\}, where M=RdM=\mathbb{R}^d, T>0T>0, and L:M×MRL:M\times M \to \mathbb{R} is a Lagrangian that is jointly convex in both variables. Under suitable conditions on the initial and final probability measures, we use convex duality \`a la Bolza and Monge-Kantorovich theory to lift classical Hopf-Lax formulae from state space to Wasserstein space. This allows us to relate optimal transport maps for the ballistic cost to those associated with the fixed-end cost defined on M×MM\times M by cT(x,y):=inf{0TL(γ(t),γ˙(t))dt,γC1([0,T),M),γ(0)=x,γ(T)=y}. c_T(x,y):=\inf\{\int_0^TL(\gamma(t), {\dot \gamma}(t))\, dt, \gamma\in C^1([0, T), M), \gamma(0)=x, \gamma(T)=y\}. We also point to links with the theory of mean field games.

Keywords

Cite

@article{arxiv.1705.05951,
  title  = {Optimal Ballistic Transport and Hopf-Lax Formulae on Wasserstein Space},
  author = {Nassif Ghoussoub},
  journal= {arXiv preprint arXiv:1705.05951},
  year   = {2017}
}

Comments

25 pages, Updated version - if any - can be downloaded at http://www.birs.ca/~nassif/