Resonance Frequencies of a Slab with Subwavelength Slits: a Fourier-transformation Approach

TL;DR

This paper introduces a rigorous Fourier-transformation method to accurately determine resonance frequencies of a conducting slab with multiple subwavelength slits, improving upon existing results with higher precision.

Contribution

It develops a novel asymptotic formula for resonance frequencies of multi-slit slabs, validated by rigorous analysis and applicable to multiple slit configurations.

Findings

Resonance frequencies are characterized by a rank-deficient linear system.

The derived formula achieves ${ m O}(h^3 \log h)$ accuracy, surpassing previous results.

Imaginary parts of resonance frequencies are ${ m O}(h)$ regardless of slit placement.

Abstract

This paper proposes a novel, rigorous and simple Fourier-transformation approach to study resonances in a perfectly conducting slab with finite number of subwavelength slits of width $h\ll 1$. Since regions outside the slits are variable separated, by Fourier transforming the governing equation, we could express field in the outer regions in terms of field derivatives on the aperture. Next, in each slit where variable separation is still available, wave field could be expressed as a Fourier series in terms of a countable basis functions with unknown Fourier coefficients. Finally, by matching field on the aperture, we establish a linear system of infinite number of equations governing the countable Fourier coefficients. By carefully asymptotic analysis of each entry of the coefficient matrix, we rigorously show that, by removing only a finite number of rows and columns, the resulting principle sub-matrix is diagonally dominant so that the infinite dimensional linear system can be reduced to a finite dimensional linear system. Resonance frequencies are exactly those frequencies making the linear system rank-deficient. This in turn provides a simple, asymptotic formula describing resonance frequencies with accuracy ${\cal O}(h^3\log h)$. We emphasize that such a formula is more accurate than all existing results and is the first accurate result especially for slits of number more than two to our best knowledge. Moreover, this asymptotic formula rigorously confirms a fact that the imaginary part of resonance frequencies is always ${\cal O}(h)$ no matter how we place the slits as long as they are spaced by distances independent of width $h$.