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Sep 8, 2023 at 20:09 comment added leo monsaingeon @Redeldio: up to some normalization yes, since they are only defined up to additive constants
Sep 8, 2023 at 16:45 comment added Redeldio @leomonsaingeon Thank you! And obviously, they are also uniformly bounded with a bound which depends only on $c$, right?
Sep 8, 2023 at 7:55 comment added leo monsaingeon For more comments I suggest you check F. Santambrogio's book [Optimal Transport for Applied Mathematicians], in partcular box 1.8 page 11 and subsequent discussions.
Sep 8, 2023 at 7:54 comment added leo monsaingeon @Redeldio : this is because a pair of Kantorovich potentials can always be taken to be c-transforms of each other, i-e $(\phi,\psi)=(\phi,\phi^c)=(\phi^{cc},\phi^c)$ so that $\phi=(\phi^c)$ is itself a c-transform. And by definition a c-transform has the same modulus of continuity as the cost function $c$. So in bounded domain a smooth cost (such as the Euclidean one) is globally Lipschitz, and therefore so is the KP. An other way to think of this is that $T(x)-x=\nabla\phi(x)$, so in bounded domains $x,T(x)\in\Omega$ are bounded and therefore so is $\nabla\phi(x)$
Sep 7, 2023 at 15:40 comment added Redeldio @leomonsaingeon You said "Indeed a Kantorovich potential $\varphi$ is always Lipschitz (at least in bounded domains)". Why? Can you tell me a reference where to find such a result? Thank you
Dec 20, 2022 at 8:54 comment added Akira @leomonsaingeon I have a question about Theorem 1.17 here. If you don't mind, please have a check in it.
Jun 18, 2022 at 22:22 answer added Shayan Hundrieser timeline score: 4
Jun 13, 2022 at 11:29 comment added JHM @leomonsaingeon If the potentials are locally Lipschitz on $\Omega$, and their restrictions to $\partial \Omega$ are also locally Lipschitz, then Alexandrov theorem (applied to $\Omega$, $\partial \Omega$) would give a.e. uniqueneness with respect to $\mathcal{L}^d|_\Omega$ and $\mathcal{L}^{d-1}|_{\partial \Omega}$. I'm sure that's obvious to you, and therefore the gradients of the max Kantorovich potentials are a.e. uniquely defined by the OT. But pointwise uniqueness of $\phi, \psi$ is more difficult, and I don't know any references.
Jun 12, 2022 at 13:12 comment added leo monsaingeon Thank you Loren. Old TeXing habits die hard, I had not noticed the spurious spacing.
Jun 12, 2022 at 13:05 comment added LSpice MathJax note: a $\newcommand\…{…}$ followed by a newline produces a spurious space in the rendered post. Distasteful as it is, one must run them together: $\newcommand\…{…}$Following text. I have edited accordingly.
Jun 12, 2022 at 13:04 history edited LSpice CC BY-SA 4.0
Capitalise title; correct spurious space
Jun 12, 2022 at 13:02 history edited Nawaf Bou-Rabee CC BY-SA 4.0
added a link to the reference
Jun 12, 2022 at 12:56 history edited leo monsaingeon CC BY-SA 4.0
fixed typos, added the missing reference
Jun 12, 2022 at 5:04 comment added leo monsaingeon @JHM: I have my own application in mind, thank you very much. I just think it is not really worth explaining here (some nonstandard parabolic problem, formally a Wasserstein gradient flow). For the technical aspect: I need to take a first variation (Fréchet derivative) $\frac{\delta W^2(\mu,\nu)}{\delta\mu}$ with respect to $\mu$ ($\nu$ being fixed). IF the Kantorovich potential is unique then this first variation is indeed given by (the flat, $L^2$ action of) $\varphi_\mu$. Before bothering someone in person I though it was worth trying here on math.MO
Jun 10, 2022 at 14:11 comment added JHM You have uniqueness of the Monge OT plan $\pi$, and in your setting the uniqueness of the subdifferentials of the dual Kantorovich potentials $\phi, \psi$. So why trouble yourself with uniqueness of the potentials themselves. Honestly why? It's very complicated question and IMO a waste of time. Are you just curious, or looking for research project, or do you have an actual application in mind? I would politely ask Jun Kitagawa or Robert McCann or Brendan Pass, if they know the answer. I've never seen them on MO.
Jun 9, 2022 at 13:18 history asked leo monsaingeon CC BY-SA 4.0