Abstract:This paper is concerned with the analysis of time-harmonic electromagnetic scattering from plasmonic inclusions in the finite frequency regime beyond the quasi-static approximation. The electric permittivity and magnetic permeability in the inclusions are allowed to be negative-valued. Using layer potential techniques for the full Maxwell system, the scattering problem is reformulated into a system of integral equations. We derive the complete eigensystem of the involved matrix-valued integral operator within … Show more
“…In fact, in many of the existing studies on plasmon resonances, the quasi-static approximation has played a critical role where the plasmonic inclusion is of a size much smaller than the wavelength. There are also several studies that go beyond the quasi-static limit [33,21,27,30,36]. In [33], double negative materials are employed in the shell and in [36], in addition to the employment of double negative materials, a so-called double-complementary medium structure is incorporated into the construction of the plasmonic device.…”
Section: Introductionmentioning
confidence: 99%
“…In [21], it is actually shown that resonance does not occur for the classical core-shell plasmonic structure without the quasistatic approximation as long as the core and shell are strictly convex. In [27,30], in order for the plasmon resonances to occur beyond the quasi-static approximation, the corresponding plasmonic configuration has to be designed in a subtle and delicate way. Nevertheless, we show that for a plasmonic structure that is resonant in the quasi-static regime but non-resonant out of the quasi-static regime, the resonance always occurs locally near a high-curvature boundary point of the plasmonic inclusion.…”
This paper reports some novel and intriguing discoveries about the localization and geometrization phenomenon in plasmon resonances and the intrinsic geometric structures of Neumann-Poincaré eigenfunctions. It is known that plasmon resonance generically occurs in the quasi-static regime where the size of the plasmonic inclusion is sufficiently small compared to the wavelength. In this paper, we show that the global smallness condition on the plasmonic inclusion can be replaced by a local high-curvature condition, and the plasmon resonance occurs locally near the high-curvature point of the plasmonic inclusion. We provide partial theoretical explanation and link with the geometric structures of the Neumann-Poincaré (NP) eigenfunctions. The spectrum of the Neumann-Poincaré operator has received significant attentions in the literature. We show for the first time some intrinsic geometric structures of the Neumann-Poincaré eigenfunctions near high-curvature points.
“…In fact, in many of the existing studies on plasmon resonances, the quasi-static approximation has played a critical role where the plasmonic inclusion is of a size much smaller than the wavelength. There are also several studies that go beyond the quasi-static limit [33,21,27,30,36]. In [33], double negative materials are employed in the shell and in [36], in addition to the employment of double negative materials, a so-called double-complementary medium structure is incorporated into the construction of the plasmonic device.…”
Section: Introductionmentioning
confidence: 99%
“…In [21], it is actually shown that resonance does not occur for the classical core-shell plasmonic structure without the quasistatic approximation as long as the core and shell are strictly convex. In [27,30], in order for the plasmon resonances to occur beyond the quasi-static approximation, the corresponding plasmonic configuration has to be designed in a subtle and delicate way. Nevertheless, we show that for a plasmonic structure that is resonant in the quasi-static regime but non-resonant out of the quasi-static regime, the resonance always occurs locally near a high-curvature boundary point of the plasmonic inclusion.…”
This paper reports some novel and intriguing discoveries about the localization and geometrization phenomenon in plasmon resonances and the intrinsic geometric structures of Neumann-Poincaré eigenfunctions. It is known that plasmon resonance generically occurs in the quasi-static regime where the size of the plasmonic inclusion is sufficiently small compared to the wavelength. In this paper, we show that the global smallness condition on the plasmonic inclusion can be replaced by a local high-curvature condition, and the plasmon resonance occurs locally near the high-curvature point of the plasmonic inclusion. We provide partial theoretical explanation and link with the geometric structures of the Neumann-Poincaré (NP) eigenfunctions. The spectrum of the Neumann-Poincaré operator has received significant attentions in the literature. We show for the first time some intrinsic geometric structures of the Neumann-Poincaré eigenfunctions near high-curvature points.
“…Recently, spectral of Neumann‐Poincaré operator has attracted much attention, for its applications in plasmon resonance, cloaking because of anomalous localized resonance, and enhancement of near cloaking . We also refer to Helsing, Kang, and Lim and Kang et al for analysis of spectral of Neumann‐Poincaré operator in domains with corners.…”
Section: Introductionmentioning
confidence: 99%
“…Most of the studies are based on the static (quasistatic) case, ie, conductivity problem. In the studies of Kang et al, Li et al, and Li and Liu, the authors consider the spectral of Neumann‐Poincaré operator in Helmholtz system with finite frequency and use the result to analyze plasmon resonance and cloaking because of anomalous localized resonance phenomena. Mathematically, one consider the following Helmholtz system.…”
In this paper, we are concerned with the asymptotic behavior of the Neumann-Poincaré operator in Helmholtz system. By analyzing the asymptotic behavior of spherical Bessel function near the origin and/or approach higher order, we prove the asymptotic behavior of spectral of Neumann-Poincaré operator when frequency is small enough and/or the order is large enough. The results show that spectral of Neumann-Poincaré operator is continuous at the origin and converges to 0 from the complex plane in general.
KEYWORDSasymptotic behavior, Helmholtz system, Neumann-Poincaré operator, spectral analysis 942
“…The CALR has been extensively investigated. We refer to [4,6,9,11,15,20,21,29] for the relevant study in acoustics, [8,10,17,18,19,27,28,24] for elastic system and [3,2,1,7,13,14,15,25,26,31,32,33,34,36,37,38] for the Maxwell system.…”
We consider the anomalous localized resonance induced by negative elastic metamaterials and its application in invisibility cloaking. We survey the recent mathematical developments in the literature and discuss two mathematical strategies that have been developed for tackling this peculiar resonance phenomenon. The first one is the spectral method, which explores the anomalous localized resonance through investigating the spectral system of the associated Neumann-Poincaré operator. The other one is the variational method, which considers the anomalous localized resonance via calculating the nontrivial kernels of a non-elliptic partial differential operator. The advantages and the relationship between the two methods are discussed. Finally, we propose some open problems for the future study.
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