2018
DOI: 10.1016/j.ijleo.2017.10.003
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FDTD analysis of diffraction efficiency in a hologram for application in optical fiber communication

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Cited by 7 publications
(3 citation statements)
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“…In addition, the iterative update of the electromagnetic field in the 3D FDTD algorithm also needs to satisfy the stability condition 45,46 :…”
Section: Finite Difference Time Domain Algorithmmentioning
confidence: 99%
See 1 more Smart Citation
“…In addition, the iterative update of the electromagnetic field in the 3D FDTD algorithm also needs to satisfy the stability condition 45,46 :…”
Section: Finite Difference Time Domain Algorithmmentioning
confidence: 99%
“…In addition, the iterative update of the electromagnetic field in the 3D FDTD algorithm also needs to satisfy the stability condition 45,46 : normalΔtbadbreak<0true1cΔx2+Δy2+Δz20.33em.$$\begin{equation} \def\eqcellsep{&}\begin{array}{*{20}{c}} {\Delta t &lt; \dfrac{1}{{c\sqrt {\Delta {x}^2 + \Delta {y}^2 + \Delta {z}^2} }}\ } \end{array} .\end{equation}$$…”
Section: Modeling and Simulationmentioning
confidence: 99%
“…[4] When employing a fine mesh during the simulation, the corresponding time step will become too small, resulting in an extremely long duration. [5] To alleviate such conditions, several unconditionally stable algorithms have been introduced to remove the CFL condition and to improve the efficiency, including alternating-direction-implicit, locally 1D, split-step procedures. [6][7][8] Notably, these are implemented by sub-step procedures to obtain the updated field components that significantly affect the accuracy and efficiency.…”
Section: Introductionmentioning
confidence: 99%