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   <subfield code="a">Ground and Bound State Solutions of Semilinear Time-Harmonic Maxwell Equations in a Bounded Domain</subfield>
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   <subfield code="c">[Thomas Bartsch, Jarosław Mederski]</subfield>
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   <subfield code="a">We find solutions $${E : \Omega \to \mathbb{R}^3}$$ E : Ω → R 3 of the problem $$\left\{\begin{aligned}&amp;\nabla \times(\nabla \times E) + \lambda E = \partial_E F(x, E) &amp;&amp;\quad \text{in }\quad \Omega \\&amp; \nu \times E = 0 &amp;&amp;\quad \text{on }\quad \partial \Omega \end{aligned} \right.$$ ∇ × ( ∇ × E ) + λ E = ∂ E F ( x , E ) in Ω ν × E = 0 on ∂ Ω on a simply connected, smooth, bounded domain $${\Omega \subset \mathbb{R}^3}$$ Ω ⊂ R 3 with connected boundary and exterior normal $${\nu : \partial \Omega \to \mathbb{R}^3}$$ ν : ∂ Ω → R 3 . Here $${\nabla \times}$$ ∇ × denotes the curl operator in $${\mathbb{R}^3}$$ R 3 , the nonlinearity $${F : \Omega \times \mathbb{R}^3 \to \mathbb{R}}$$ F : Ω × R 3 → R is superquadratic and subcritical in E. The model nonlinearity is of the form $${F(x, E)=\Gamma(x) |E|^p}$$ F ( x , E ) = Γ ( x ) | E | p for $${\Gamma \in L^\infty(\Omega)}$$ Γ ∈ L ∞ ( Ω ) positive, some 2&lt;p&lt;6. It need not be radial nor even in the E-variable. The problem comes from the time-harmonic Maxwell equations, the boundary conditions are those for Ω surrounded by a perfect conductor.</subfield>
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   <subfield code="a">Bartsch</subfield>
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   <subfield code="u">Mathematisches Institut, Universität Giessen, Arndtstr. 2, 35392, Giessen, Germany</subfield>
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