Abstract

A one-dimensional plasma medium is playing a crucial role in modern sensing device design, which can benefit significantly from numerical electromagnetic wave simulation. In this study, we introduce a novel lattice Boltzmann scheme with a single extended force term for electromagnetic wave propagation in a one-dimensional plasma medium. This method is developed by reconstructing the solution to the macroscopic Maxwell’s equations recovered from the lattice Boltzmann equation. The final formulation of the lattice Boltzmann scheme involves only the equilibrium and one non-equilibrium force term. Among them, the former is calculated from the macroscopic electromagnetic variables, and the latter is evaluated from the dispersive effect. Thus, the proposed lattice Boltzmann scheme directly tracks the evolution of macroscopic electromagnetic variables, which yields lower memory costs and facilitates the implementation of physical boundary conditions. Detailed conduction is carried out based on the Chapman–Enskog expansion technique to prove the mathematical consistency between the proposed lattice Boltzmann scheme and Maxwell’s equations. Based on the proposed method, we present electromagnetic pulse propagating behaviors in nondispersive media and the response of a one-dimensional plasma slab to incident electromagnetic waves that span regions above and below the plasma frequency ωp, and further investigate the optical properties of a one-dimensional plasma photonic crystal with periodic thin layers of plasma with different layer thicknesses to verify the stability, accuracy, and flexibility of the proposed method.

Highlights

  • Plasma media have been widely used in current photonic topological insulator studies [1–3], in one-dimensional (1D) plasma photonic crystals (PhCs) [4–7], two-dimensional (2D) PhCs [8,9], and three-dimensional (3D) PhC construction

  • Owing to the advantages of 1D plasma medium applications, researchers are strongly motivated to investigate the electromagnetic response on plasma dispersive media to design more efficient 1D PhCs sensing devices

  • We introduce a different expression form for the Maxwell’s equation in an isotropic dispersive medium and propose a new frequency-dependent lattice Boltzmann method (LBM) with only a single extended force term (LBM-SEF) for electromagnetic waves propagation in a plasma medium

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Summary

Introduction

Plasma media have been widely used in current photonic topological insulator studies [1–3], in one-dimensional (1D) plasma photonic crystals (PhCs) [4–7], two-dimensional (2D) PhCs [8,9], and three-dimensional (3D) PhC construction. Owing to their complex design and manufacturing, the potential applications of topological photonics in 2D and 3D PhCs are very limited. PhCs have been employed to manipulate the light-matter interactions by tuning the plasma layer thickness in PhCs. Owing to the advantages of 1D plasma medium applications, researchers are strongly motivated to investigate the electromagnetic response on plasma dispersive media to design more efficient 1D PhCs sensing devices. Several numerical methods have been proposed to solve the electromagnetic (EM) wave propagation problem [12–14]

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