横向磁性 ENZ 谐振器:鲁棒性和最佳形状设计

IF 2.6 1区 数学 Q1 MATHEMATICS, APPLIED Archive for Rational Mechanics and Analysis Pub Date : 2024-11-06 DOI:10.1007/s00205-024-02023-6
Robert V. Kohn, Raghavendra Venkatraman
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引用次数: 0

摘要

我们研究的是 Liberal、Mahmoud 和 Engheta 在 2016 年《自然-通讯》论文中提出的某些 "几何不变谐振腔"。它们是使用麦克斯韦方程的横向磁还原建模的圆柱形装置,因此数学是二维的。其横截面由一个电介质包含体组成,周围是一个 "ε-近零"(ENZ)外壳。当外壳的面积恰到好处时,它与介质的相互作用就会产生共振。从数学上讲,共振是二维发散形式赫尔莫耳茨方程 \(\nabla \cdot \left( \varepsilon ^{-1}(x,\omega ) \nabla u \right) + \omega ^2 \mu u = 0\) 的非微观解,其中 \(\varepsilon (x. \omega ) \) 是 "ε-近零"(ENZ)壳的非微观解、\)是(复值)介电常数,\(\omega \)是频率,\(\mu \)是磁导率,并且在外壳的外部边界施加了均质诺伊曼条件。这是一个非线性特征值问题,因为 \(\varepsilon \) 取决于 \(\omega \)。在外壳中使用 ENZ 材料意味着 \(\varepsilon (x,\omega )\) 在那里几乎为零,所以 PDE 是相当奇异的。我们使用洛伦兹模型来研究ENZ材料的弥散,通过证明当洛伦兹模型的损耗参数足够小时存在预期的共振,将利伯尔等人的讨论建立在坚实的基础之上。我们的分析是微扰性质的,尽管 PDE 的形式显然是奇异的,但我们使用了隐函数定理。虽然共振的存在只取决于 ENZ 外壳的面积,但其质量(即共振衰减的速度)却取决于外壳的形状。因此,我们很自然地要考虑一个相关的优化设计问题:哪种形状的外壳能产生衰减最慢的共振?我们证明,如果介质内含物是一个球,那么最佳外壳就是一个同心环形。对于任何形状的包含体,我们利用凸对偶工具研究了设计问题的凸松弛。最后,我们讨论了一个猜想,即我们的松弛问题等同于考虑近似最优设计的同质化极限。
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Transverse Magnetic ENZ Resonators: Robustness and Optimal Shape Design

We study certain “geometric-invariant resonant cavities” introduced by Liberal, Mahmoud, and Engheta in a 2016 Nature Communications paper. They are cylindrical devices modeled using the transverse magnetic reduction of Maxwell’s equations, so the mathematics is two-dimensional. The cross-section consists of a dielectric inclusion surrounded by an “epsilon-near-zero” (ENZ) shell. When the shell has just the right area, its interaction with the inclusion produces a resonance. Mathematically, the resonance is a nontrivial solution of a 2D divergence-form Helmoltz equation \(\nabla \cdot \left( \varepsilon ^{-1}(x,\omega ) \nabla u \right) + \omega ^2 \mu u = 0\), where \(\varepsilon (x,\omega )\) is the (complex-valued) dielectric permittivity, \(\omega \) is the frequency, \(\mu \) is the magnetic permeability, and a homogeneous Neumann condition is imposed at the outer boundary of the shell. This is a nonlinear eigenvalue problem, since \(\varepsilon \) depends on \(\omega \). Use of an ENZ material in the shell means that \(\varepsilon (x,\omega )\) is nearly zero there, so the PDE is rather singular. Working with a Lorentz model for the dispersion of the ENZ material, we put the discussion of Liberal et. al. on a sound foundation by proving the existence of the anticipated resonance when the loss parameter of the Lorentz model is sufficiently small. Our analysis is perturbative in character, using the implicit function theorem despite the apparently singular form of the PDE. While the existence of the resonance depends only on the area of the ENZ shell, its quality (that is, the rate at which the resonance decays) depends on the shape of the shell. It is therefore natural to consider an associated optimal design problem: what shape shell gives the slowest-decaying resonance? We prove that if the dielectric inclusion is a ball then the optimal shell is a concentric annulus. For an inclusion of any shape, we study a convex relaxation of the design problem using tools from convex duality. Finally, we discuss the conjecture that our relaxed problem amounts to considering homogenization-like limits of nearly optimal designs.

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来源期刊
CiteScore
5.10
自引率
8.00%
发文量
98
审稿时长
4-8 weeks
期刊介绍: The Archive for Rational Mechanics and Analysis nourishes the discipline of mechanics as a deductive, mathematical science in the classical tradition and promotes analysis, particularly in the context of application. Its purpose is to give rapid and full publication to research of exceptional moment, depth and permanence.
期刊最新文献
A Top-Down Approach to Algebraic Renormalization in Regularity Structures Based on Multi-indices Homogenisation Problems for Free Discontinuity Functionals with Bounded Cohesive Surface Terms Transverse Magnetic ENZ Resonators: Robustness and Optimal Shape Design The Equality Case in the Substatic Heintze–Karcher Inequality Regularity and compactness for critical points of degenerate polyconvex energies
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