Trajectory Stabilization of Nonlocal Continuity Equations by Localized Controls

We discuss stabilization around trajectories of the continuity equation with nonlo cal vector fields, where the control is localized, i.e., it acts on a fixed subset of the configuration space. We first show that the correct definition of stabilization is the following: given an initial error of order epsilon , measured in Wasserstein distance, one can improve the final error to an order epsilon (1+kappa) with kappa > 0. We then prove the main result: assuming that the trajectory crosses the subset of control action, stabilization can be achieved. The key problem lies in regularity issues: the reference trajectory needs to be absolutely continuous, while the initial state to be stabilized needs to be realized by a small Lipschitz perturbation or by being in a very small neighborhood of it.

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Publication Details

Journal
SIAM Journal on Control and Optimization
Published
2024-12-13
DOI
https://doi.org/10.1137/24m1644274
Citations
1
Primary Topic
Advanced Mathematical Physics Problems
Type
article
Field-Weighted Citation Impact
0.89
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article

Trajectory Stabilization of Nonlocal Continuity Equations by Localized Controls

Nikolay Pogodaev, Francesco Rossi
1 citations
SIAM Journal on Control and Optimization
Advanced Mathematical Physics Problems
0.89
article

Trajectory Stabilization of Nonlocal Continuity Equations by Localized Controls

Nikolay Pogodaev, Francesco Rossi
article en
1 citations

Abstract

We discuss stabilization around trajectories of the continuity equation with nonlo cal vector fields, where the control is localized, i.e., it acts on a fixed subset of the configuration space. We first show that the correct definition of stabilization is the following: given an initial error of order epsilon , measured in Wasserstein distance, one can improve the final error to an order epsilon (1+kappa) with kappa > 0. We then prove the main result: assuming that the trajectory crosses the subset of control action, stabilization can be achieved. The key problem lies in regularity issues: the reference trajectory needs to be absolutely continuous, while the initial state to be stabilized needs to be realized by a small Lipschitz perturbation or by being in a very small neighborhood of it.

SIAM Journal on Control and OptimizationVol. 62(6)
University of Padua (IT)
Openalex Percentile: Top 25%
Advanced Mathematical Physics Problems
0.89
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