Indicatrix of TE and TM- polarized wave velocities in crystal of classes 4mm, 3m, 6mm with magneto-electric effect

IF 0.4 Q4 PHYSICS, MULTIDISCIPLINARY Bulletin of the University of Karaganda-Physics Pub Date : 2023-03-30 DOI:10.31489/2023ph1/23-30
S. Tleukenov, Zh. N. Suierkulova, S. Nurkenov
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Abstract

This work is devoted to the theoretical study of the laws of propagation of electromagnetic waves of TE and TM polarization in anisotropic media belonging to classes 4mm, 3m, 6mm, etc. having a magnetoelectric effect. The directions of the vectors of the phase and group velocities of the polarization waves TE and TM at the boundary of a uniaxial crystal with magnetoelectric properties are considered. In the analytical form, the values of the directions of the phase and group velocities of the TE and TM waves are indicated, depending on the direction of the wave vector of the incident wave. The consequences of the obtained results for uniaxial crystals in the absence of magnetoelectric properties are discussed. The solution of the tasks set in this paper is based on the use of the matrix method. On its basis, various problems of wave processes in an isotropic elastic medium, electromagnetic waves in crystals, the distribution of coupled elastic and electromagnetic waves in piezoelectric and piezomagnetic media with a magnetoelectric effect were previously considered. In the presence of a magnetoelectric effect for electromagnetic waves propagating through uniaxial crystals, the parameters of the wave vector, phase and group velocities are determined. The obtained results are analyzed for electromagnetic waves propagating through uniaxial crystals in the absence of a magnetoelectric effect. The indicatrices of the wave vectors propagating in the plane and the phase velocities of the TM polarization waves are limited ( 0 ) x z . Based on the Rayleigh equation, the values of the group velocity are obtained. The density of electromagnetic energy fluxes and their components are determined for TE and TM waves. The energy transfer rate and its direction are determined. It is shown that the group velocities and directions obtained from the Rayleigh equation and the Umov-Poynting vector do not coincide.
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具有磁电效应的4mm、3m、6mm级晶体中TE和TM偏振波速度的指示线
本论文从理论上研究了TE和TM极化电磁波在4mm、3m、6mm等各向异性介质中具有磁电效应的传播规律。考虑了具有磁电性质的单轴晶体边界处极化波TE和TM的相速度矢量和群速度矢量的方向。在解析形式中,根据入射波的波矢量方向,表示了TE波和TM波的相速度和群速度方向的值。讨论了在没有磁电性质的情况下,所得结果对单轴晶体的影响。本文的任务集的求解基于矩阵法的应用。在此基础上,前人研究了各向同性弹性介质中的波过程、晶体中的电磁波、具有磁电效应的压电和压磁介质中耦合的弹性和电磁波的分布等问题。在电磁波在单轴晶体中传播时存在磁电效应的情况下,确定了波矢量、相速度和群速度的参数。分析了电磁波在没有磁电效应的情况下通过单轴晶体传播的结果。在平面上传播的波矢量的指标和TM偏振波的相速度是有限的(0)x z。根据瑞利方程,得到了群速度的数值。确定了TE波和TM波的电磁能量通量密度及其分量。确定了能量传递速率及其方向。结果表明,由瑞利方程得到的群速度和群方向与Umov-Poynting矢量不重合。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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