Slide 18
Slide 18 text
Transport Bregman Properties
(i) Non-negativity: Suppose F is displacement convex, then
DT,F
(p q) ≥ 0.
Suppose F is strictly displacement convex, then
DT,F
(p q) = 0 if and only if DistT
(p, q) = 0.
(ii) Transport Hessian metric: Consider a Taylor expansion as follows.
Denote σ = −∇ · (q∇Φ) ∈ Tq
P(Ω) and ∈ R, then
DT,F
((id + ∇Φ)#
q q) =
2
2
HessT
F(q)(σ, σ) + o( 2),
where id: Ω → Ω is the identical map, id(x) = x, and HessT
F(q) is
the Hessian operator of functional F at q ∈ P(Ω) w.r.t.
L2–Wasserstein metric.
(iii) Asymmetry: In general, DT,F
(p q) = DT,F
(q p).
Our transport duality relates to mean field game’s Wasserstein
Hamilton-Jacobi equation (Big mac).
18