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MAXWELL'S EQUATIONS AS A SCATTERING PASSIVE LINEAR SYSTEM?

机译:MAXWELL方程作为散射被动线性系统?

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We consider Maxwell's equations on a bounded domain Ω ? R~3 with Lipschitz boundary Γ, with boundary control and boundary observation. Relying on an abstract framework developed by us in an earlier paper, we define a scattering passive linear system that corresponds to Maxwell's equations and investigate its properties. The state of the system is [_D~B], where B and D are the magnetic and electric flux densities, and the state space of the system is X = E?E, where E = L~2(Ω;R~3). We assume that Γ0 and Γ1 are disjoint, relatively open subsets of Γ such that Γ_0∪Γ_1 = Γ. We consider Γ_0 to be a superconductor, which means that on Γ_0 the tangential component of the electric field is forced to be zero. The input and output space U consists of tangential vector fields of class L~2 on Γ_1. The input and output at any moment are suitable linear combinations of the tangential components of the electric and magnetic fields. The semigroup generator has the structure A =[L~ 0·G-γ~(-L)?Rγ ]P, where L = rot (with a suitable domain), γ is the tangential component trace operator restricted to Γ1, R is a strictly positive pointwise multiplication operator on U (that can be chosen arbitrarily), and P~(-1) = [ ~(μ 0)_(0 ε)] is another strictly positive pointwise multiplication operator (acting on X). The operator -G is pointwise multiplication with the conductivity g ≥ 0 of the material in Ω. The system is scattering conservative iff g = 0.
机译:我们考虑有限域Ω上的麦克斯韦方程。 R〜3具有Lipschitz边界Γ,具有边界控制和边界观察。依靠我们在较早的论文中开发的抽象框架,我们定义了一个与麦克斯韦方程组相对应的散射无源线性系统,并研究了其性质。系统的状态为[_D〜B],其中B和D为磁通密度和电通量密度,系统的状态空间为X = E?E,其中E = L〜2(Ω; R〜3 )。我们假设Γ0和Γ1是Γ的不相交,相对开放的子集,使得Γ_0∪Γ_1=Γ。我们认为Γ_0是超导体,这意味着在Γ_0上,电场的切向分量被迫为零。输入和输出空间U由Γ_1上L〜2类的切向矢量场组成。任何时候的输入和输出都是电场和磁场的切向分量的合适线性组合。半群生成器的结构为A = [L〜0·G-γ〜(-L)?Rγ] P,其中L = rot(具有合适的域),γ是切线分量跟踪算子,其限制为Γ1,R为U上的一个严格正的逐点乘法算子(可以任意选择),并且P〜(-1)= [〜(μ0)_(0ε)]是另一个严格的正的逐点乘法算子(作用于X)。算子-G是按点乘以材料的电导率g≥0(以Ω为单位)。系统在i = 0时保守散射。

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