Search arXiv⌕ Search

arXiv · 2610.39829

Klein-Gordon-Born-Infeld equations driven by mixed local-nonlocal operators

Abstract

In this paper we study a class of Klein-Gordon-Born-Infeld systems in which the classical Laplacian appearing in the matter equation is replaced by a mixed local-nonlocal operator, whose nonlocal part is allowed to be nonpositive definite according to a real parameter. Both the approximate and the exact Born-Infeld field equations are considered in parallel. After making the functional framework explicit, we identify a range of real parameters for which infinitely many radially symmetric standing waves exist, obtained as Mountain Pass critical points of the associated reduced energy functionals. The mixed local-nonlocal operator reduces to the classical Laplacian as the nonlocal weight vanishes, and is motivated, in the spirit of effective field theories, by nonlocal corrections to the matter dispersion relation.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Nicolò Cangiotti, Maicol Caponi, Alberto Maione, Enzo Vitillaro. 2026-10-29. Klein-Gordon-Born-Infeld equations driven by mixed local-nonlocal operators. https://arxiv.org/abs/2610.39829

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Linear stability analysis for 2D shear flows near Couette in the isentropic Compressible Euler equations

In this paper, we investigate linear stability properties of the 2D isentropic compressible Euler equations linearized around a shear flow given by a monotone profile, close to the Couette flow, with constant density, in the domain $\mathbb{T}\times \mathbb{R}$. We begin by directly investigating the Couette shear flow, where we characterize the linear growth of the compressible part of the fluid while proving time decay for the incompressible part (inviscid damping with slower rates). Then we extend the analysis to monotone shear flows near Couette, where we are able to give an upper bound, superlinear in time, for the compressible part of the fluid. The incompressible part enjoys an inviscid damping property, analogous to the Couette case. In the pure Couette case, we exploit the presence of an additional conservation law (which connects the vorticity and the density on the moving frame) in order to reduce the number of degrees of freedom of the system. The result then follows by using weighted energy estimates. In the general case, unfortunately, this conservation law no longer holds. Therefore we define a suitable weighted energy functional for the whole system, which can be used to estimate the irrotational component of the velocity but does not provide sharp bounds on the solenoidal component. However, even in the absence of the aforementioned additional conservation law, we are still able to show the existence of a functional relation which allows us to recover somehow the vorticity from the density, on the moving frame. By combining the weighted energy estimates with the functional relation we also recover the inviscid damping for the solenoidal component of the velocity.

math.AP↗

The evolution equation and the eigenvalue problem for the Laplacian in a regular tree

In this paper, our main goal is to study the evolution problem associated with the Laplacian operator with Dirichlet boundary conditions on a regular tree. To this end, we place special emphasis on the associated first eigenvalue problem, which provides the fundamental tool for describing the long-time dynamics. First, we prove existence and uniqueness of solutions when the initial condition is compatible with the boundary condition. Next, we address the asymptotic behavior of the solutions and show that they decay to zero exponentially fast. This decay rate is determined by the associated first eigenvalue, which we also analyze in detail.

math.AP↗

Invariant Densities on Cylinders with an Interface: Existence, Uniqueness, and Exponential Asymptotics

We study the stationary double-divergence equation on the infinite cylinder $\mathbb R\times\mathbb T^{d-1}$, whose coefficients coincide with two possibly different periodic media outside a bounded interface layer. Under the centering conditions for the two periodic media, we construct a positive invariant density that converges exponentially in $C^1$ at each end to a positive multiple of the corresponding periodic invariant density. Every bounded distributional solution is a scalar multiple of this density. The two asymptotic amplitudes are determined by the full interface problem, up to a common normalization. Motivated by the invariant-measure analysis of Hairer and Manson [Ann. Probab. 39(2011) 648-682], our proof uses only PDE methods: a transformation based on the periodic invariant densities, adjoint Neumann problems on finite cylinders, and energy estimates.

math.AP↗