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   <subfield code="u">Faculty of Mathematics and Computer Science, Nicolaus Copernicus University, ul. Chopina 12/18, 87-100, Toruń, Poland</subfield>
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   <subfield code="a">Ground States of Time-Harmonic Semilinear Maxwell Equations in $${\mathbb{R}^3}$$ R 3 with Vanishing Permittivity</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[Jarosław Mederski]</subfield>
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   <subfield code="a">We investigate the existence of solutions $${E:\mathbb{R}^3 \to \mathbb{R}^3}$$ E : R 3 → R 3 of the time-harmonic semilinear Maxwell equation $$\nabla \times (\nabla \times E) + V(x) E = \partial_E F(x, E) \quad {\rm in} \mathbb{R}^3$$ ∇ × ( ∇ × E ) + V ( x ) E = ∂ E F ( x , E ) in R 3 where $${V:\mathbb{R}^3 \to \mathbb{R}}$$ V : R 3 → R , $${V(x) \leqq 0}$$ V ( x ) ≦ 0 almost everywhere on $${\mathbb{R}^3}$$ R 3 , $${\nabla \times}$$ ∇ × denotes the curl operator in $${\mathbb{R}^3}$$ R 3 and $${F:\mathbb{R}^3 \times \mathbb{R}^3 \to \mathbb{R}}$$ F : R 3 × R 3 → R is a nonlinear function in E. In particular we find a ground state solution provided that suitable growth conditions on F are imposed and the $${L^{3/2}}$$ L 3 / 2 -norm of V is less than the best Sobolev constant. In applications, F is responsible for the nonlinear polarization and $${V(x) = -\mu\omega^2 \varepsilon(x)}$$ V ( x ) = - μ ω 2 ε ( x ) whereμ&gt;0 is the magnetic permeability, ω is the frequency of the time-harmonic electric field $${\mathfrak{R}\{E(x){\rm e}^{i\omega t}\}}$$ R { E ( x ) e i ω t } and $${\varepsilon}$$ ε is the linear part of the permittivity in an inhomogeneous medium.</subfield>
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   <subfield code="a">Metadata rights reserved</subfield>
   <subfield code="b">Springer special CC-BY-NC licence</subfield>
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