Saved in:
Bibliographic Details
Main Authors: Kohn, Robert V., Venkatraman, Raghavendra
Format: Preprint
Published: 2024
Subjects:
Online Access:https://arxiv.org/abs/2403.11242
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1866910499345530880
author Kohn, Robert V.
Venkatraman, Raghavendra
author_facet Kohn, Robert V.
Venkatraman, Raghavendra
contents We study certain "geometric-invariant resonant cavitie"' introduced by Liberal et. al in a 2016 Nature Comm. paper, modeled using the transverse magnetic reduction of Maxwell's equations. The cross-section consists of a dielectric inclusion surrounded by an "epsilon-near-zero" (ENZ) shell. When the shell has 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 $\nabla \cdot \left(\varepsilon^{-1}(x,ω) \nabla u \right) + ω^2 μu = 0$, where $\varepsilon(x,ω)$ is the (complex-valued) dielectric permittivity, $ω$ is the frequency, $μ$ 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 $ω$. Use of an ENZ material in the shell means that $\varepsilon(x,ω)$ 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 is sufficiently small. Our analysis is perturbative in character despite the apparently singular form of the PDE. While the existence of the resonance depends only on the area of the ENZ shell, the rate at which it decays depends on the shape of the shell. We 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, and discuss the conjecture that our relaxed problem amounts to considering homogenization-like limits of nearly optimal designs.
format Preprint
id arxiv_https___arxiv_org_abs_2403_11242
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Transverse Magnetic ENZ Resonators: Robustness and Optimal Shape Design
Kohn, Robert V.
Venkatraman, Raghavendra
Analysis of PDEs
Spectral Theory
Optics
We study certain "geometric-invariant resonant cavitie"' introduced by Liberal et. al in a 2016 Nature Comm. paper, modeled using the transverse magnetic reduction of Maxwell's equations. The cross-section consists of a dielectric inclusion surrounded by an "epsilon-near-zero" (ENZ) shell. When the shell has 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 $\nabla \cdot \left(\varepsilon^{-1}(x,ω) \nabla u \right) + ω^2 μu = 0$, where $\varepsilon(x,ω)$ is the (complex-valued) dielectric permittivity, $ω$ is the frequency, $μ$ 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 $ω$. Use of an ENZ material in the shell means that $\varepsilon(x,ω)$ 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 is sufficiently small. Our analysis is perturbative in character despite the apparently singular form of the PDE. While the existence of the resonance depends only on the area of the ENZ shell, the rate at which it decays depends on the shape of the shell. We 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, and discuss the conjecture that our relaxed problem amounts to considering homogenization-like limits of nearly optimal designs.
title Transverse Magnetic ENZ Resonators: Robustness and Optimal Shape Design
topic Analysis of PDEs
Spectral Theory
Optics
url https://arxiv.org/abs/2403.11242