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Comparison of Cartesian grid configurations for application of the finite-difference time-domain method to electromagnetic scattering by dielectric particles

机译:有限差分时域方法在介电粒子电磁散射中的笛卡尔网格配置比较

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摘要

Two grid configurations can be employed to implement the finite-difference time-domain (FDTD) technique in a Cartesian system. One configuration defines the electric and magnetic field components at the cell edges and cell-face centers, respectively, whereas the other reverses these definitions. These two grid configurations differ in terms of implication on the electromagnetic boundary conditions if the scatterer in the FDTD computation is a dielectric particle. The permittivity has an abrupt transition at the cell interface if the dielectric properties of two adjacent cells are not identical. Similarly, the discontinuity of permittivity is also observed at the edges of neighboring cells that are different in terms of their dielectric constants. We present two FDTD schemes for light scattering by dielectric particles to overcome the above-mentioned discontinuity on the basis of the electromagnetic boundary conditions for the two Cartesian grid configurations. We also present an empirical approach to accelerate the convergence of the discrete Fourier transform to obtain the field values in the frequency domain. As a new application of the FDTD method, we investigate the scattering properties of multibranched bulletrosette ice crystals at both visible and thermal infrared wavelengths.
机译:可以采用两个网格配置在笛卡尔系统中实现时域有限差分(FDTD)技术。一种配置分别在单元边缘和单元面中心定义了电场和磁场分量,而另一种配置则颠倒了这些定义。如果FDTD计算中的散射体是电介质粒子,则这两个网格结构在对电磁边界条件的影响方面会有所不同。如果两个相邻单元的介电特性不同,则介电常数在单元界面处会突然转变。类似地,在介电常数不同的相邻单元的边缘处也观察到介电常数的不连续性。我们针对两种直角网格结构的电磁边界条件,提出了两种FDTD方案,用于通过介电粒子进行光散射,以克服上述不连续性。我们还提出了一种经验方法来加速离散傅立叶变换的收敛,以获得频域中的场值。作为FDTD方法的一种新应用,我们研究了多分支子弹头冰晶在可见光和热红外波长下的散射特性。

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