共查询到17条相似文献,搜索用时 265 毫秒
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基于面积分方程的矩量法及其快速算法研究了复杂含核粒子对任意入射贝塞尔波束的散射特性.将零阶贝塞尔束的矢量解和坐标系旋转理论相结合,推导出任意入射贝塞尔波束电磁场分量的数学表达式.根据等效原理,建立了求解具有任意形状和复杂内部结构含核粒子散射问题的面积分方程.对贝塞尔波束任意入射下一些复杂含核粒子的散射进行了数值模拟,结果表明:贝塞尔波束入射时的微分散射截面要小于平面波入射时的微分散射截面,且随着半锥角的减小而增大;当波束中心的位置远离粒子中心时,微分散射截面会减小;微分散射截面对波束的入射角非常敏感.这为激光对微粒的探测、诊断以及操纵技术提供有益帮助. 相似文献
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基于电磁场的矢量波函数展开方法和不同坐标系中矢量波函数转化关系,得到了圆对称矢量贝塞尔涡旋波束的圆柱矢量波函数展开系数;结合电磁场边界条件,获得了圆对称矢量贝塞尔涡旋波束以任意方向照射均匀单轴各向异性介质层的反射场、透射场和内部场的展开系数;数值计算了沿波束传播方向横截面上的入射、反射和透射电场强度分布以及xOz平面内传播路径方向的总电场强度分布。结果表明,圆对称贝塞尔涡旋波束入射单轴各向异性介质的反射场基本保持同心圆环结构,但强度分布不再呈圆对称;透射场出现两束交错折射光,总电场强度轮廓显著扭曲。 相似文献
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基于广义洛伦兹-米理论,研究两个聚焦的高斯光束沿着任意方向入射单轴各向异性涂层球的散射特性。基于球矢量波函数的正交特性,推导得到双高斯光束的球矢量波函数展开表达式。通过引入傅里叶变换,求解得到各向异性涂层区域内的电磁场展开式,将涂层球各区域的电磁场用球矢量波函数展开,再结合边界条件,得到沿任意方向传播的双高斯光束入射到涂层球的散射系数和雷达散射截面。数值模拟了雷达散射截面随散射角变化的分布,将单轴各向异性涂层球退化为单轴各向异性球时的散射结果与文献进行对比,结果十分吻合。分析双光束的入射角、粒子内半径、涂层厚度与内半径的比值、电和磁各向异性对散射强度及其散射角分布的影响。该理论和数值分析能够为激光对涂层颗粒的探测、散射以及光学操作提供有益帮助。 相似文献
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基于广义Mie理论, 研究了椭球粒子对在轴入射的拉盖尔-高斯光束的散射特性. 通过局域近似法求解椭球坐标系中的波束因子, 计算得到了波束因子之间满足的普遍关系. 对散射强度随椭球粒子不同尺寸参数和扁圆程度的变化特性进行了数值计算, 并针对不同拓扑荷时的散射强度进行了对比分析. 结果表明: 当椭球粒子尺寸在与入射光波长可比拟的范围内变化时, 散射强度随尺寸参数的增大而增大, 随椭球长短轴之比和拓扑荷的增大而减小. 本文的理论研究能够为拉盖尔-高斯光束在粒径测量、大气激光通信、 大气遥感等领域的应用提供更准确的粒子模型和参考价值.
关键词:
椭球粒子
拉盖尔-高斯光束
波束因子
散射强度 相似文献
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An approach to express an incident shaped beam with respect to an arbitrarily oriented spheroidal particle having layers with non-confocal boundaries is presented. To overcome the difficulty of non-confocal boundary conditions connected with different spheroidal coordinate systems, a theoretical procedure is developed to deal with the non-confocal boundary conditions by virtue of a transformation for vector wave functions. The unknown coefficients of scattered and internal electromagnetic fields are determined by solving a system of linear equations derived from the boundary conditions and relations between the spheroidal vector wave functions and spherical ones. Numerical results of the normalized scattering cross section for a two-layered non-confocal prolate spheroid are evaluated. PACS 42.25.Fx; 42.25.Bs 相似文献
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The generalized Lorenz-Mie theory in the strict sense describes the interaction between an illuminating arbitrary shaped beam and a homogeneous sphere characterized by its diameter d and its complex refractive index m. It relies on the method of separation of variables expressed in spherical coordinates. Other generalized Lorenz-Mie theories (for other kinds of scatterers) expressed in spherical coordinates are available too. In these theories, the illuminating beam is expressed by using expansions with expansion coefficients depending on some fundamental coefficients named beam shape coefficients, more specifically spherical beam shape coefficients. In this paper we present a general formulation for the transformation of spherical beam shape coefficients through rotations of coordinate systems. 相似文献
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Z.W. Cui Y.P. Han J.J. Wang W.J. Zhao 《Journal of Quantitative Spectroscopy & Radiative Transfer》2012,113(6):480-488
A hybrid finite element-boundary integral method is applied to characterize the scattering of an arbitrarily incident-focused Gaussian beam by arbitrarily shaped inhomogeneous particles. Specifically, the Davis–Barton fifth-order approximation in combination with rotation Euler angles is used to represent the arbitrarily incident Gaussian beams. The finite element method is employed to formulate the fields in the interior region of the inhomogeneous particle, while the boundary integral equation is applied to represent the fields in the exterior region. The interior and exterior fields are coupled by means of the field continuity conditions. To reduce the computational burden, the frontal method and the multilevel fast multipole algorithm are adopted to solve the resultant matrix equation. Numerical results for differential scattering cross sections of several selected inhomogeneous particles are presented and can be served as further study on this subject. 相似文献
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Yiping Han Yang Zhang Huayong Zhang Guoxia Han 《Journal of Quantitative Spectroscopy & Radiative Transfer》2009,110(14-16):1375-1381
The expansions of the incident arbitrary beam shape in spherical, spheroidal and cylindrical coordinates in the general case of oblique illumination are presented. The scattered electromagnetic fields of typical particles of arbitrary orientation illuminated with a beam shape are provided. The numerical results of the normalized scattering cross section are evaluated. 相似文献
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