2014
DOI: 10.1016/j.camwa.2013.03.005
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Numerical realization of Dirichlet-to-Neumann transparent boundary conditions for photonic crystal wave-guides

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Cited by 9 publications
(31 citation statements)
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“…This eigenvalue problem is linear in ω 2 when fixing k ∈ B, the so called ω-formulation, and quadratic in k when fixing ω ∈ R + , the so called k-formulation. However, note that this problem is posed on the unbounded domain S. Now let us come to the spectral properties of (2.3) as shown in [5,13], which are relevant for this work. For any k ∈ B we will denote the set of frequencies ω 2 for which Bloch modes [14] in the PhC + PhC on top or in the PhC − PhC below the defect exist by σ ess (k) ⊂ R + .…”
Section: Transformation To Periodic Problem and Spectral Propertiesmentioning
confidence: 99%
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“…This eigenvalue problem is linear in ω 2 when fixing k ∈ B, the so called ω-formulation, and quadratic in k when fixing ω ∈ R + , the so called k-formulation. However, note that this problem is posed on the unbounded domain S. Now let us come to the spectral properties of (2.3) as shown in [5,13], which are relevant for this work. For any k ∈ B we will denote the set of frequencies ω 2 for which Bloch modes [14] in the PhC + PhC on top or in the PhC − PhC below the defect exist by σ ess (k) ⊂ R + .…”
Section: Transformation To Periodic Problem and Spectral Propertiesmentioning
confidence: 99%
“…For more details and proofs the reader is referred to [5,13]. Before we can present the spectral properties we need to introduce several function spaces.…”
Section: Transformation To Periodic Problem and Spectral Propertiesmentioning
confidence: 99%
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