2011
DOI: 10.2528/pierm11012501
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Efficient Simulations of Periodic Structures With Oblique Incidence Using Direct Spectral FDTD Method

Abstract: A simple and efficient joint algorithm of finite difference time domain (FDTD) and periodic boundary condition (PBC), called as the direct spectral FDTD method, has been investigated to study three-dimensional (3D) periodic structures with oblique incidence, where both the azimuth angle φ and the elevation angle θ are varying. The number of sampling points for the horizontal wave number can be determined by using an adaptive approach. As numerical results, the transmission and reflection coefficients from spli… Show more

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Cited by 8 publications
(5 citation statements)
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“…Some modification of this technique is required to simulate periodic structures for the case of oblique incidence. In this case, the incident field can be written as the signal evolution recorded during a preliminary FDTD simulation [42,43] or a packet of plane waves with fixed in-plane wave vector [44,45]. The last modification is used within the hybrid FDTD transfer matrix method as well [46].…”
Section: A Field-partitioning Approachmentioning
confidence: 99%
“…Some modification of this technique is required to simulate periodic structures for the case of oblique incidence. In this case, the incident field can be written as the signal evolution recorded during a preliminary FDTD simulation [42,43] or a packet of plane waves with fixed in-plane wave vector [44,45]. The last modification is used within the hybrid FDTD transfer matrix method as well [46].…”
Section: A Field-partitioning Approachmentioning
confidence: 99%
“…Our method can be combined with the existing FDTD methods for simulation of periodic structures at the oblique incidence [42][43][44][45][46][47][48][49][50]. For example, the transfer matrix may be calculated as described above for an obliquely incident plane wave, which can be simulated using an iterative technique [42,43].…”
Section: Discussionmentioning
confidence: 99%
“…Let us assume a (l x , l y ) periodicity in the (x, y) directions with a z-propagation of an incident wave. Like [10], an arbitrary azimuth angle is chosen to ϕ = ϕ 0 . Then, the horizontal wavenumber depends on the angular frequency ω = 2πf and the elevation angle θ as k h = ω sin θ/c 0 .…”
Section: Spectral Fdtd Reviewmentioning
confidence: 99%