Ground and Bound State Solutions of Semilinear Time-Harmonic Maxwell Equations in a Bounded Domain

Verfasser / Beitragende:
[Thomas Bartsch, Jarosław Mederski]
Ort, Verlag, Jahr:
2015
Enthalten in:
Archive for Rational Mechanics and Analysis, 215/1(2015-01-01), 283-306
Format:
Artikel (online)
ID: 605515182
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024 7 0 |a 10.1007/s00205-014-0778-1  |2 doi 
035 |a (NATIONALLICENCE)springer-10.1007/s00205-014-0778-1 
245 0 0 |a Ground and Bound State Solutions of Semilinear Time-Harmonic Maxwell Equations in a Bounded Domain  |h [Elektronische Daten]  |c [Thomas Bartsch, Jarosław Mederski] 
520 3 |a We find solutions $${E : \Omega \to \mathbb{R}^3}$$ E : Ω → R 3 of the problem $$\left\{\begin{aligned}&\nabla \times(\nabla \times E) + \lambda E = \partial_E F(x, E) &&\quad \text{in }\quad \Omega \\& \nu \times E = 0 &&\quad \text{on }\quad \partial \Omega \end{aligned} \right.$$ ∇ × ( ∇ × 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
540 |a Springer-Verlag Berlin Heidelberg, 2014 
700 1 |a Bartsch  |D Thomas  |u Mathematisches Institut, Universität Giessen, Arndtstr. 2, 35392, Giessen, Germany  |4 aut 
700 1 |a Mederski  |D Jarosław  |u Faculty of Mathematics and Computer Science, Nicolaus Copernicus University, ul. Chopina 12/18, 87-100, Toruń, Poland  |4 aut 
773 0 |t Archive for Rational Mechanics and Analysis  |d Springer Berlin Heidelberg  |g 215/1(2015-01-01), 283-306  |x 0003-9527  |q 215:1<283  |1 2015  |2 215  |o 205 
856 4 0 |u https://doi.org/10.1007/s00205-014-0778-1  |q text/html  |z Onlinezugriff via DOI 
898 |a BK010053  |b XK010053  |c XK010000 
900 7 |a Metadata rights reserved  |b Springer special CC-BY-NC licence  |2 nationallicence 
908 |D 1  |a research-article  |2 jats 
949 |B NATIONALLICENCE  |F NATIONALLICENCE  |b NL-springer 
950 |B NATIONALLICENCE  |P 856  |E 40  |u https://doi.org/10.1007/s00205-014-0778-1  |q text/html  |z Onlinezugriff via DOI 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Bartsch  |D Thomas  |u Mathematisches Institut, Universität Giessen, Arndtstr. 2, 35392, Giessen, Germany  |4 aut 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Mederski  |D Jarosław  |u Faculty of Mathematics and Computer Science, Nicolaus Copernicus University, ul. Chopina 12/18, 87-100, Toruń, Poland  |4 aut 
950 |B NATIONALLICENCE  |P 773  |E 0-  |t Archive for Rational Mechanics and Analysis  |d Springer Berlin Heidelberg  |g 215/1(2015-01-01), 283-306  |x 0003-9527  |q 215:1<283  |1 2015  |2 215  |o 205