2017
DOI: 10.1007/s00605-017-1037-y
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Gradient flows of time-dependent functionals in metric spaces and applications to PDEs

Abstract: We develop a gradient-flow theory for time-dependent functionals defined in abstract metric spaces. Global well-posedness and asymptotic behavior of solutions are provided. Conditions on functionals and metric spaces allow to consider the Wasserstein space P 2 (R d ) and apply the results for a large class of PDEs with time-dependent coefficients like confinement and interaction potentials and diffusion. Our results can be seen as an extension of those in Ambrosio- Gigli-Savaré (2005)[2] to the case of timedep… Show more

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Cited by 11 publications
(31 citation statements)
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“…In [23], where general non-convex problems have been studied, a certain Lipschitz condition for the free energy functional comes into play which resembles our additional conditions on h from (M4). In [9,23], re-proving the classical properties of the minimizing movement scheme is more involved than for our scheme from Definition 1.2-in contrast, deriving higher regularity estimates brings additional difficulties in our case, since now the heat entropy is a time-dependent functional. Non-autonomous equations of Wasserstein gradient flow form with linear mobility have also been investigated in [22] using a time-averaged form of the classical minimizing movement scheme.…”
Section: 2mentioning
confidence: 95%
See 1 more Smart Citation
“…In [23], where general non-convex problems have been studied, a certain Lipschitz condition for the free energy functional comes into play which resembles our additional conditions on h from (M4). In [9,23], re-proving the classical properties of the minimizing movement scheme is more involved than for our scheme from Definition 1.2-in contrast, deriving higher regularity estimates brings additional difficulties in our case, since now the heat entropy is a time-dependent functional. Non-autonomous equations of Wasserstein gradient flow form with linear mobility have also been investigated in [22] using a time-averaged form of the classical minimizing movement scheme.…”
Section: 2mentioning
confidence: 95%
“…This auxiliary flow is-by construction-the heat flow. Nonautonomous evolution equations of gradient flow type have already been studied in [9,23] from the opposite point of view: there, time-dependent energy functionals on time-independent metric spaces were considered and a different modification of the minimizing movement scheme was investigated. In [23], where general non-convex problems have been studied, a certain Lipschitz condition for the free energy functional comes into play which resembles our additional conditions on h from (M4).…”
Section: 2mentioning
confidence: 99%
“…To circumvent this problem we suppose that the set of differentiability points can be chosen independent of x, cf. [10,21]. To illustrate this we give the following example, which has also been discussed in [21].…”
Section: Dynamic Edi-and Ede-gradient Flowsmentioning
confidence: 99%
“…Unlike in the static case we additionally have to impose a condition on the difference quotients of the functionals, cf. [10,Theorem 5.4].…”
Section: Dynamic Edi-and Ede-gradient Flowsmentioning
confidence: 99%
“…This was the starting point of interpretations of more general nonlinear, nonlocal Fokker-Planck equations as Wasserstein gradient flows with respect to time-dependent energies, on constrained manifolds and even of none dissipative equations. A selection of works introducing certain constraints into gradient flows are [11,6,21].…”
Section: Introductionmentioning
confidence: 99%