2008
DOI: 10.1016/j.jcp.2008.01.029
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A periodic FMM for Maxwell’s equations in 3D and its applications to problems related to photonic crystals

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Cited by 59 publications
(84 citation statements)
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“…These have a rigorous mathematical foundation [11,34], and have the advantages of discretizing the material interfaces alone, of automatically enforcing radiation conditions, and of high-order convergence, which allows high accuracies to be reached very efficiently. The standard way to adapt integral equations to solve periodic scattering problems is by replacing the free-space kernel (see (2.7)) by the quasi-periodic Green's function (the kernel appearing in (3.4) with P = ∞); see [35,36,43]. Considerable effort has been spent on the tricky task of computing this quasiperiodic Green's function efficiently (see, for example, [3,12,25,28,31]).…”
Section: Introduction and Problem Formulationmentioning
confidence: 99%
See 1 more Smart Citation
“…These have a rigorous mathematical foundation [11,34], and have the advantages of discretizing the material interfaces alone, of automatically enforcing radiation conditions, and of high-order convergence, which allows high accuracies to be reached very efficiently. The standard way to adapt integral equations to solve periodic scattering problems is by replacing the free-space kernel (see (2.7)) by the quasi-periodic Green's function (the kernel appearing in (3.4) with P = ∞); see [35,36,43]. Considerable effort has been spent on the tricky task of computing this quasiperiodic Green's function efficiently (see, for example, [3,12,25,28,31]).…”
Section: Introduction and Problem Formulationmentioning
confidence: 99%
“…In the related case of periodic surface scattering, Zhang and Chandler-Wilde [47] modified the Green's function to that of a half-space, which cures this divergence (this was implemented in [2]); however, this idea fails to help in our case of disconnected obstacles. A final problem is that the quasi-periodic Green's function is often computed using lattice sums [25,26], which is natural when using fast multipole acceleration in large-scale scattering problems [36]. However, since this representation converges in discs (or spheres in 3D), it becomes cumbersome for high aspect ratio geometries.…”
Section: Introduction and Problem Formulationmentioning
confidence: 99%
“…Stabilization of MLFMA for low-frequency applications has attracted the interest of many researchers, leading to development of diverse approaches to solve the low-frequency breakdown problem [12][13][14][15][16][17][18][19][20][21][22][23]. In one approach, spectral representation of the Green's function is used so that electromagnetic waves are divided into propagating and evanescent parts [12][13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…In general, when the Maxwell equations are numerically solved in a large-scale system, the fast multipole method, which is the boundary element method to which multipole expansion is applied, is well used, where, in the boundary element method, the differential equations, i.e., the Maxwell equations, are transformed into an integral equation by means of a tensor Green function. The periodic FMM is a numerical method whose Green function is extended for the case that scattering domains exist periodically in a system (Otani and Nishimura, 2008). In the periodic FMM, a system which is finite in the direction stacking layers, i.e., x-direction, but infinite in the y-and z-directions is considered.…”
Section: Numerical Methods and Numerical Modelmentioning
confidence: 99%