arXiv:2104.02341 [math.AP]AbstractReferencesReviewsResources
Weyl formula for the eigenvalues of the dissipative acoustic operator
Published 2021-04-06Version 1
We study the wave equation in the exterior of a bounded domain $K$ with dissipative boundary condition $\partial_{\nu} u - \gamma(x) u = 0$ on the boundary $\Gamma$ and $\gamma(x) > 0.$ The solutions are described by a contraction semigroup $V(t) = e^{tG}, \: t \geq 0.$ The eigenvalues $\lambda_k$ of $G$ with ${\rm Re}\: \lambda_k < 0$ yield asymptotically disappearing solutions $u(t, x) = e^{\lambda_k t} f(x)$ having exponentially decreasing global energy. We establish a Weyl formula for these eigenvalues in the case $\min_{x\in \Gamma} \gamma(x) > 1.$ For strictly convex obstacles $K$ this formula concerns all eigenvalues of $G.$
Related articles: Most relevant | Search more
arXiv:2310.01192 [math.AP] (Published 2023-10-02)
Eigenvalues and resonances of dissipative acoustic operator for strictly convex obstacles
arXiv:0706.0350 [math.AP] (Published 2007-06-04)
Decay and non-decay of the local energy for the wave equation in the De Sitter - Schwarzschild metric
arXiv:1506.02555 [math.AP] (Published 2015-06-08)
Eigenvalues for Maxwell's equations with dissipative boundary conditions