2017
DOI: 10.1137/16m1056560
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A Fully Discrete Variational Scheme for Solving Nonlinear Fokker--Planck Equations in Multiple Space Dimensions

Abstract: We introduce a novel spatio-temporal discretization for nonlinear Fokker-Planck equations on the multi-dimensional unit cube. This discretization is based on two structural properties of these equations: the first is the representation as a gradient flow of an entropy functional in the L 2 -Wasserstein metric, the second is the Lagrangian nature, meaning that solutions can be written as the push forward transformation of the initial density under suitable flow maps. The resulting numerical scheme is entropy di… Show more

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Cited by 38 publications
(45 citation statements)
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“…Since µ n 1 = µ n + c n 2 (µ n 1 − µ n 2 ), µ n 2 = µ n + c n 1 (µ n 2 − µ n 1 ), we deduce from (72) the desired L 2 ((0, T ); L q d (Ω)) estimates on the phase potentials µ n i with q d defined in Definition 2.3. Finally, the combination of the relations (36), (27), (53) and (41) yields…”
Section: Flow Interchange and Entropy Estimatementioning
confidence: 99%
“…Since µ n 1 = µ n + c n 2 (µ n 1 − µ n 2 ), µ n 2 = µ n + c n 1 (µ n 2 − µ n 1 ), we deduce from (72) the desired L 2 ((0, T ); L q d (Ω)) estimates on the phase potentials µ n i with q d defined in Definition 2.3. Finally, the combination of the relations (36), (27), (53) and (41) yields…”
Section: Flow Interchange and Entropy Estimatementioning
confidence: 99%
“…A common approach is to go to the Lagrangian formulation, using that the optimal γ is typically concentrated on the graph of a transport map T : Ω → Ω. This is extremely efficient in one space dimension [7,22,23], but becomes significantly more cumbersome -and difficult to analyze -in multiple dimensions [5,12,13,18]. Various alternatives to the Lagrangian approach are available, including finite volume methods [21], blob methods [11] etc.…”
Section: Discretization and Regularizationmentioning
confidence: 99%
“…The approximate solution inherits automatically positivity, mass conservation and energy dissipation. Different approaches to actually compute the minimizers of (1.4) have been investigated: particle schemes [6,8,7,38]; evolving diffeomorphisms [8,10]; Lagrangian schemes [3,12,14,19,26,28]; entropic regularization [31]. However, it turns out that the application of these schemes to gradient flows in L 2 -Wasserstein space is intricate, since computing the L 2 -Wasserstein distance and its gradient is difficult in dimension two or more.…”
Section: Introductionmentioning
confidence: 99%