A quasilinear transmission problem with application to Maxwell equations with a divergence-free $\mathcal{D}$-field

Abstract

Maxwell equations in the absence of free charges require initial data with a divergence free displacement field $\mathcal{D}$. In materials in which the dependence $\mathcal{D}=\mathcal{D}(\mathcal{E})$ is nonlinear the quasilinear problem $\nabla \cdot \mathcal{D}(\mathcal{E})=0$ is hence to be solved. In many applications, e.g. in the modelling of wave-packets, an approximative asymptotic ansatz of the electric field $\mathcal{E}$ is used, which satisfies this divergence condition at $t=0$ only up to a small residual. We search then for a small correction of the ansatz to enforce $\nabla \cdot \mathcal{D}(\mathcal{E})=0$ at $t=0$ and choose this correction in the form of a gradient field. In the usual case of a power type nonlinearity in $\mathcal{D}(\mathcal{E})$ this leads to the sum of the Laplace and $p$-Laplace operators. We also allow for the medium to consist of two different materials so that a transmission problem across an interface is produced. We prove the existence of the correction term for a general class of nonlinearities and provide regularity estimates for its derivatives, independent of the $L^2$-norm of the original ansatz. In this way, when applied to the wave-packet setting, the correction term is indeed asymptotically smaller than the original ansatz. We also provide numerical experiments to support our analysis.

30 pages, 8 figures

References in corpus (2)

• Ginzburg-Landau equation bound to the metal-dielectric interface and transverse nonlinear optics with amplified plasmon polaritons
• Existence and qualitative theory for nonlinear elliptic systems with a nonlinear interface condition used in electrochemistry