Spectral problems for non elliptic symmetric systems with dissipative boundary conditions

preprint2014arXivOpen access

Abstract

This paper considers and extends spectral and scattering theory to dissipative symmetric systems that may have zero speeds and in particular to strictly dissipative boundary conditions for Maxwell's equations. Consider symmetric systems ∂t−∑j=1nAj∂xj\partial_t - \sum_{j=1}^n A_j \partial_{x_j} in Rn, n≥3{\mathbb R}^n,\: n \geq 3, nn odd, in a smooth connected exterior domain Ω:=Rn∖KˉΩ:= {\mathbb R}^n \setminus \bar{K}. Assume that the rank of A(ξ)=∑j=1nAjξjA(ξ) = \sum_{j= 1}^n A_j ξ_j is constant for ξ≠0.ξ\not= 0. For maximally dissipative boundary conditions on Ω:=Rn∖KˉΩ:={\mathbb R}^n \setminus \bar{K} with bounded open domain KK the solution of the boundary problem in R+×Ω{\mathbb R}^{+} \times Ω is described by a contraction semigroup V(t)=etGb, t≥0.V(t) = e^{t G_b},\:t \geq 0. Assuming coercive conditions for GbG_b and its adjoint Gb∗G_b^* on the complement of their kernels, we prove that the spectrum of GbG_b in the open half plane ℜz<0\Re z < 0 is formed only by isolated eigenvalues with finite multiplicities.

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