“…Substituting the field values in (17a) using (17b), as well as those of the polarization currents from the expressions derived in the previous section, the following update equation is derived: (18) The coefficients indicated in (18) are as follows: (19) Equation (18) is converted into a tridiagonal system with respect to the electric field nodal values at time step throughout the grid, with system matrix . .…”
Section: B Adi-fdtd Based On the Ade Methodsmentioning
confidence: 99%
“…To characterize the dispersion of the corresponding infinite periodic structure in the linear regime, one unit cell with both layers chosen to be linear, i.e., , is analyzed using periodic boundary conditions, implemented via the sine-cosine method [19]. Fig.…”
Section: Spatial Solitons In a Nonlinear Bragg Reflectormentioning
“…Substituting the field values in (17a) using (17b), as well as those of the polarization currents from the expressions derived in the previous section, the following update equation is derived: (18) The coefficients indicated in (18) are as follows: (19) Equation (18) is converted into a tridiagonal system with respect to the electric field nodal values at time step throughout the grid, with system matrix . .…”
Section: B Adi-fdtd Based On the Ade Methodsmentioning
confidence: 99%
“…To characterize the dispersion of the corresponding infinite periodic structure in the linear regime, one unit cell with both layers chosen to be linear, i.e., , is analyzed using periodic boundary conditions, implemented via the sine-cosine method [19]. Fig.…”
Section: Spatial Solitons In a Nonlinear Bragg Reflectormentioning
“…The transverse termination is provided by imposing periodic boundary conditions (PBC). In the practical implementation of the PBC, the sin-cos dual plane-wave excitation (dual-time source) is developed in (12) , where the enforcement of the phase shift due to the periodicity is made straightforward.…”
Section: Light Wave Analysis By Fdtd Methodsmentioning
To realize wider viewing angle for a liquid-crystal display (LCD), particular attention is being paid to the in-plane switching (IPS) mode of LCD, where pixel electrodes and common (opposite) electrodes are arranged on the same array substrate and liquid crystal is made respond by an electric field generated in parallel to the substrate. So far, two types of array electrode structures are proposed in IPS-LCD. One is the array structure with two electrode layers where pixel electrodes and common electrodes are formed on different conductive layers. In the other array structure they are formed on one conductive layer. Although both electrode structures of IPS-LCD have problems dependent on the process conditions, light leakage observed only in the former structure along the edge of the common electrodes at zero bias is an essentially serious problem. By studying light wave propagation in the IPS-LCD using a two-dimensional finite-difference timedomain method we have found that the light leakage is caused by the tapered side surfaces of the common electrodes.
“…Various techniques have been proposed in literature in order to analyze frequency selective surfaces (FSS) (Bardi et al, 2002;Bozzi & Perregrini, 1999;Harms et al, 1994;Mittra et al, 1988;Wu, 1995). The standard method of moments (MoM) approach is based on the induced electric currents on the FSS but it can be prohibitively costly from a computational point of view, if not even impractical in some cases, and this could explain why MoM is so unpopular.…”
Section: Single and Multi-layer Ebg Full-wave Analysismentioning
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