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首页> 外文期刊>Optics Communications: A Journal Devoted to the Rapid Publication of Short Contributions in the Field of Optics and Interaction of Light with Matter >Electromagnetic eigenoscillations and fields in a dielectric microsphere with multilayer spherical stack
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Electromagnetic eigenoscillations and fields in a dielectric microsphere with multilayer spherical stack

机译:具有多层球体堆叠的介电微球体中的电磁本征振荡和场

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We analyze numerically the spectrum of the eigenfrequencies and the electromagnetic eigenfields distribution in the spherical microsphere coated by the multilayered dielectric spherical stack in the optical frequency range. The general eigenfrequency equation is derived. The eigenfrequencies values are calculated versus the number of layers in the stack. We have found what Q factor can reach the large values for the eigenfrequency in the range of strong reflectivity of the stack (stop band). The eigenfrequencies laying beyond the stop band are unstable with respect to changing the number of layers, and such frequencies have low Q factors. The eigenfrequencies inside stop band are stable and their Q factors exponentially increase with the growth of the number of layers in stack until the saturation because of an influence of material losses in layers. The explicit calculation of the radial distribution of the electromagnetic eigenfields confirms that the energy of field is concentrated in the deepest part of the layered system. The confinement of the energy of optical eigenoscillations takes place in such states. The field amplitudes of oscillations decrease exponentially with a removal from the center of resonator up to external boundary. Therefore, the influence of the nonlinearity must be most substantial in the central part of the dielectric microsphere. We analyze several representative geometries: a dielectric sphere, a metallic sphere with the deposited stack on both of them.
机译:我们在光学频率范围内数值分析了多层介电球形叠层包覆的球形微球的本征频谱和电磁本征场分布。推导了一般的本征频率方程。计算特征频率值相对于堆叠中的层数。我们发现在堆栈的强反射率(阻带)范围内,什么Q因子可以达到本征频率的较大值。就改变层数而言,超出阻带的本征频率不稳定,并且此类频率的Q因子较低。由于层中材料损失的影响,阻带内的本征频率是稳定的,并且它们的Q因子随着堆叠中层数的增加呈指数增长,直到达到饱和为止。电磁本征场径向分布的显式计算证实了场能量集中在分层系统的最深部分。在这种状态下发生光学本征振荡能量的限制。随着从谐振腔中心到外部边界的移动,振荡的场振幅呈指数下降。因此,非线性的影响在电介质微球的中心部分必须是最大的。我们分析了几种具有代表性的几何形状:介电球,金属球以及在两者上均沉积有堆叠的金属。

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