NANAFAOCMar 20

A new comparison principle for discrete Volterra equations with an application to convex sweeping processes with infinite delays

arXiv:2603.2008952.0h-index: 12
Predicted impact top 73% in NA · last 90 daysOriginality Incremental advance
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This work addresses a theoretical gap in discrete approximations for delayed sweeping processes, which is incremental but important for numerical analysis in control and optimization.

The paper tackles the problem of establishing uniform bounds for discrete Volterra equations, which is crucial for proving compactness in convex sweeping processes with infinite delays, and demonstrates through numerical simulations that the projected point can be at O(1) distance from the boundary.

Comparison principles for Volterra equations play a role analogous to maximum principles in PDEs: they provide positivity and stability information on the solution and allow one to control the output of bounded inputs. In the continuous setting, such results often rely on Laplace-transform or spectral methods (see Gripenberg, Londen, and Staffans, Volterra Integral and Functional Equations, 1990). However, these tools are not uniform in the discretization step $h$ hence fail in discrete or semi-discrete approximations. The present note introduces a resolvent-free argument yielding uniform $L^\infty(0,T)$-bounds for non-negative kernels. Compactness is a key ingredient in order to show existence of sweeping processes. While in the classical framework it is well established, adding an infinite distribution of delays complicates greatly the obtaining of such a result. In a first step we show a general energy decay estimate, which is then used to establish compactness. The argument is carried out in the discrete setting and that necessitates the introduction of the new comparison principle. In the classical sweeping process the previous position of the particle lies on the boundary of the constraint set, staying $O(h)$ close to the next projection point ($h$ is the discretization step). Our delay model projects the particle's averaged (by a unit measure kernel) past positions to the constraint set. Numerical simulations show that the projected point can lie at $O(1)$ distance from the convex set's boundary.

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