2001
DOI: 10.1006/jcph.2001.6765
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FDFD: A 3D Finite-Difference Frequency-Domain Code for Electromagnetic Induction Tomography

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Cited by 55 publications
(46 citation statements)
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“…To address this key challenge in the design and understanding of lasers, a highly efficient approach to finding the nonlinear steady-state properties of complex laser systems has recently been introduced, known by the acronym SALT (steady-state ab initio laser theory). 1 In this paper, we present a technique to directly solve the SALT formulation [6][7][8] of the steady-state MB equations (using finite-difference frequency-domain (FDFD) [9,10] or finite-element methods (FEM) [11]), and we demonstrate that, unlike previous approaches to the SALT equations [7,8], our technique scales to full three-dimensional (3D) low-symmetry geometries (such as photonic-crystal slabs [12]). …”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…To address this key challenge in the design and understanding of lasers, a highly efficient approach to finding the nonlinear steady-state properties of complex laser systems has recently been introduced, known by the acronym SALT (steady-state ab initio laser theory). 1 In this paper, we present a technique to directly solve the SALT formulation [6][7][8] of the steady-state MB equations (using finite-difference frequency-domain (FDFD) [9,10] or finite-element methods (FEM) [11]), and we demonstrate that, unlike previous approaches to the SALT equations [7,8], our technique scales to full three-dimensional (3D) low-symmetry geometries (such as photonic-crystal slabs [12]). …”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, we show in Sec. III E that analytical outgoingradiation boundary conditions, which are difficult to generalize to three dimensions [20], can be substituted by the standard PML (perfectly matched layer) method [10,20,21] which is equally effective at modeling open systems. We also demonstrate multimode laser solutions (Secs.…”
Section: Introductionmentioning
confidence: 99%
“…III B) for these standing-mode solutions will no longer be given by the simple expressions in Eqs. (34) and (35), and will have to be numerically computed (nevertheless, we have empirically found that these standing-mode solutions are still unstable).…”
Section: Effects Of Chiralitymentioning
confidence: 99%
“…In many cases, the C nv -symmetric geometry we are trying to solve has a degeneracy that is broken when the geometry is approximated by a discretized grid for numerical solution on a computer [14,35,36] since the grid may no longer have the original C nv symmetry. For linear equations, this unphysical splitting is not an issue because it is usually straightforward to tell whether a pair of modes is "really" degenerate by how it corresponds to the eigenfunctions of the "real" symmetry group, and since all linear superpositions solve the equation in the infinite-resolution limit, we can construct arbitrary superpositions as needed after solving for both of the modes.…”
Section: C Nv Symmetry Broken By Discretizationmentioning
confidence: 99%
“…Generally speaking, it is known that in FDFD (and FDFD) methods the assignment of the material properties to the grid cells (e.g., µ i,j,k r,xx ) is a fundamental step which can be performed by various techniques [29,33,34]. In [26], the pointwise value of the constitutive parameters has been assigned to each node in the Yee grid (i.e., µ i,j,k r,xx = µ r,xx (i∆x, (j + 0.5)∆y, (k + 0.5)∆z), for example), and the discretization grid has been chosen in order to avoid that any node could lay on a discontinuity of the dielectric permittivity or of the magnetic permeability [26].…”
Section: Fdfd Discretization Of Sharp Interfacesmentioning
confidence: 99%