水平层状介质中任意方向磁偶极子的电磁场分布

将水平层状介质中的任意方向磁偶极子分解成水平磁偶极子(HMD)和垂直磁偶极子(VMD),给出了将VMD和HMD产生的波分解为电场矢量垂直于入射面的线形极化波(EV波)和平行于入射面的线形极化波(EP波)的方法.通过分别研究这两种波在各层介质中的反射和透射规律,导出确定各介质层中电磁波的递推公式,从而得到了任意介质层中电磁波的解析表达式.     

倾斜井眼中感应测井正演模拟与响应特征

感应测井仪器的发射源可简化为一系列磁偶极子,其在层状地层中产生的电磁场可分解成彼此独立的TE波和TM波叠加,且TE波和TM波完全由两个标量方程确定.首先研究倾斜井眼中磁偶极子场的TE波和TM波分解,推导多层介质中电磁场振幅以及地层界面上广义反射和透射系数的递推公式,给出层状地层电磁场解析解.然后利用数值结果分析考察砂泥岩薄交互层中,地层层厚、井眼倾角变化等对感应测井响应的影响.     

任意半径圆形电流在径向成层介质中产生的电磁场

采用递推矩阵方法计算径向成层介质中的二维Green函数.根据层界面处电场和磁场的连续性条件得到确定待定系数的矩阵方程组并通过递推方法快速求解.只需改变方程组中源项元素的位置,就可以方便地得到当源点和场点在任意层时的二维Green函数,并进而得到具有任意半径的圆形电流在介质中产生的电磁场.本文给出的Green函数具有表达方式简洁的优点.     

填充多层互易手征介质金属同轴线传播特性

 采用在圆柱坐标系中分离变量的方法，推出填充多层互易手征介质的金属同轴线各层电磁场之间的关系，得到其模式特征方程和圆波导模式特征方程，给出了填充两层手征介质金属同轴线部分模式的色散特性的数值计算结果，分析了手征介质参量及两层手征介质厚度变化等对手征同轴线传播特性的影响。如果互易手征介质的手征参数等于零，可得填充普通介质的同轴线的模式特征方程。与填充普通介质的同轴线中的模式相比，手征同轴线中的模式发生了分叉。当同轴线中所填介质的折射率增大时，其模式归一化截止频率和进行基模单模传输的带宽归一化频率都将减小。     

物质透明性质的分析

本文从经典电磁场理论出发,利用多层垂直入射的方法计算光在理想介质中的传播,进而探讨光在有损介质和金属中的传播情况,分析出电导率是导致上述介质传播光存在差异的重要原因,又从微观角度探究影响电导率的因素,得出文章结论.     

外标法NMR实验中化学位移的校正

推导了 NMR实验中任意条件下柱状介质所感受到的有效磁场和固有化学位移的公式 ,概括了通过单谱仪、双谱仪和魔角实验校正化学位移的方法 ,阐述了平行场和垂直场中的介质磁化率效应。     

用边有限元方法计算磁偶极子的三维电磁响应

用边有限元基函数导出了麦克斯韦(Maxwell)方程的有限元关系式,计算了地下三维介质中磁偶极子的电磁场响应.将场分量定义在有限单元的边上,解决了结点有限元方法中场切向分量不连续的矛盾,保证了源除外的所有单元内有旋无散的特性.将总场分离成背景场和二次场,使该方法适用于任何方向的磁偶极子源.通过模拟算例分析了7种Krylov子空间迭代算法以及不完全乔累斯基分解预处理手段在解大型线性代数方程组中的计算效率和收敛特性.对比结果表明,施加不完全乔累斯基分解作预处理的广义乘积型双共轭梯度算法GPBiCG (Pbicg)收敛最快,是三维复杂介质电磁响应数值模拟的首选算法.     

新型金属-多层绝缘介质-金属表面等离子波导结构的传输特性

设计了一种新型金属-多层绝缘介质-金属表面等离子波导结构,利用时域有限差分法对其传输特性进行数值分析。研究了有效折射率和传播长度与中间多层绝缘介质厚度之间的关系,并分析了金属层的角度对该波导结构中场分布的影响。结果表明:当光波从波导结构上方垂直入射时,电磁场被限制在多层介质中的高折射率区,实现了场的耦合传输。多层绝缘介质的厚度均为220 nm时,正六边形金属层结构对应的波导结构的传输性能较为理想。该结构能够实现亚波长尺度的光限制,可以应用于光电子集成和传感器领域。     

水平薄层包围的流体井孔中声波场的数值模拟

针对声波测井薄层探测的需要,用半解析方法求解了地层为水平多层介质时柱状井孔内脉冲点源激发的声场。通过模式解求出了层间的广义反射矩阵,使得各水平区域的场用层间的广义反射矩阵表出,最后给出了井外为。层介质的形式解,并在井外为三层介质出现一薄层时,对接收器纵向位置位于层下、层间和层上记录的波形进行了数值模拟,得到了首波波至的正确显示。讨论了薄层对波至与幅度的影响。     

多层介质对应力波传播特性影响分析

 通过在气炮上进行多层介质的低速冲击实验及相应的数值计算，分析了不同组成的多层介质对应力波传播特性的影响。结果表明：多层介质中的泡沫材料不仅能够改变应力波的幅值与作用时间，而且具有显著的吸能效果，引起应力波在传播过程中在各层介质中能量与动量分配的改变。通过对泡沫铝和泡沫混凝土两种软材料在多层介质中作用的比较表明，在低速冲击的实验条件下，含泡沫混凝土的多层介质具有较好的削波作用，含泡沫铝的多层介质具有较好的吸能性能。     

Conduction-electron spin resonance in two-dimensional structures

The influence of the conduction-electron spin magnetization density, induced in a two-dimensional electron layer by a microwave electromagnetic field, on the reflection and transmission of the field is considered. Because of the induced magnetization and electric current, both the electric and magnetic components of the field should have jumps on the layer. A way to match the waves on two sides of the layer, valid when the quasi-two-dimensional electron gas is in the one-mode state, is proposed. By following this way, the amplitudes of transmitted and reflected waves as well as the absorption coefficient are evaluated.     

Light amplification and attenuation in stratified structures with a complex refractive index

We report a new kind of laser-threshold resonance in electromagnetic wave propagation inside a layered medium. Specifically, for large values of the gain coefficient, the wave interaction with only the first few lattice interfaces results in transmission and reflection values of much greater than unity. We also show that the duality phenomenon between losses and gains on the field amplitude decay is due to the existence of counterpropagating waves on reflection from the layer interfaces.     

Reflected and refracted electromagnetic fields in a semi-infinite body

We compute the reflected and refracted electromagnetic fields for an ideal semi-infinite body (either a plasma or a dielectric), as well as the reflection coefficient, by using a general approach based on the polarization equation of motion and electromagnetic potentials. The method consists of representing the charge disturbances by a displacement field in the positions of the moving charges. The propagation of an electromagnetic wave in matter is treated by means of the retarded electromagnetic potentials, and the resulting integral equations are solved. Generalized Fresnel’s relations are thereby obtained for any incidence angle and polarization and the angles of total polarization and total reflection are derived (the latter for the plasma). Bulk and surface plasmon–polariton modes are also identified for the plasma. As it is well known, the field inside the plasma is either damped (evanescent) or propagating (transparency regime), and the reflection coefficient exhibits an abrupt enhancement on passing from the propagating regime to the damped one (total reflection).     

Reflection and refraction of the electromagnetic field in a semi-infinite plasma

We compute the reflected and refracted electromagnetic fields for an ideal semi-infinite (half-space) plasma, as well as the reflection coefficient, by using a general procedure based on equations of motion and electromagnetic potentials. The approach consists of representing the charge disturbances by a displacement field in the positions of the moving particles (electrons). The propagation of an electromagnetic wave in plasma is treated by means of the retarded electromagnetic potentials, and the resulting integral equations are solved. Generalized Fresnel’s relations are thereby obtained for any incidence angle and polarization and the angles of total polarization and total reflection are derived. Bulk and surface plasmon-polariton modes are identified. As it is well known, the field inside the plasma is either damped (evanescent) or propagating (transparency regime), and the reflection coefficient exhibits an abrupt enhancement on passing from the propagating regime to the damped one (total reflection).     

纳米金表面修饰与表面等离子体共振传感器的相互作用研究

为了分析纳米金表面修饰对表面等离子体共振(SPR)的放大作用,以及其对传感器本身的影响,首先,基于色散介质的吸收理论,通过建立波长型SPR生物传感器四层膜结构的数学模型,理论分析了传感器表面所吸附纳米金对传感器的影响:纳米金的表面修饰,改变了表面等离子体传感器中棱镜表面各介质层内电磁场的能量分布,削弱了金属膜在共振吸收中的作用,从而使SPR曲线的半波宽度增加,最小反射系数增大,金膜的最优膜厚度也随之改变.其次,通过不同厚度的金膜外吸附纳米金的对比试验,验证了此理论.金膜厚45nm、表面修饰10nm纳米金颗 关键词： 表面等离子体共振 生物传感器 纳米金 金属膜     

Light amplification and attenuation in stratified structures with a complex refractive index

Abstract

We report a new kind of laser-threshold resonance in electromagnetic wave propagation inside a layered medium. Specifically, for large values of the gain coefficient, the wave interaction with only the first few lattice interfaces results in transmission and reflection values of much greater than unity. We also show that the duality phenomenon between losses and gains on the field amplitude decay is due to the existence of counterpropagating waves on reflection from the layer interfaces.     

Faraday Rotation of Overdense Magnetized Plasma

In this study, we investigate Faraday rotation of electromagnetic waves that are anomalously transmitted through an over‐dense magnetized plasma layer. Here, magnetized plasma indicates that the plasma layer is immersed in a uniform magnetic field. Firstly, normally opaque over‐dense magnetized plasma is shown to be transparent to obliquely incident electromagnetic waves. This high transparency can be achieved by providing conditions for resonant excitations of plasmonic modes. The resonant characteristics of the transmission coefficient of the considered structure are determined and discussed. The conditions under which the magnetized plasma behaves as a complete reflector are also obtained. Faraday rotation is shown to be enhanced under high transparency conditions. The reflected wave also exhibits Faraday rotation and is enhanced under total reflection conditions. (© 2015 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

A new method to measure permittivity and permeability in nanopowder materials in microwave range

A new method for measuring the electromagnetic properties (permittivity and permeability) of nanopowder materials in a wide microwave region is presented. Unlike previously developed systems, our experimental setup is based on reflection measurements over a short-circuited transmission line combined with the application of a uniform magnetostatic field. When this field is sufficiently high to saturate the material, the effective permeability of the sample equals the permeability of free space, without modifying its electrical properties. Hence, for each frequency, the permittivity can be obtained through the measurement of a single scattering parameter, such as the reflection coefficient. After this first measurement, and once the external field is removed, the reflection coefficient can be used again to obtain the permeability by means of the permittivity value obtained before. As the major advantage, this procedure allows the recording of the experimental data in just one sweep, using one-port measurements, and without modifying the geometrical characteristics of the sample holder. Hence, the measurement process can be easily automated.     

On Reflection and Transmission of Electromagnetic Waves Obliquely Incident on Relativistically Moving Uniaxial and Isotropic Plasma Slabs

The oscillations in the power reflection coefficient as a function of the normalized slab velocity are shown for electromagnetic waves obliquely incident on a relativistically moving uniaxial plasma slab with an infinitely strong magneto-static field parallel to the slab boundaries. This paper also summarizes and concludes the sequence on the reflection and transmission of electromagnetic waves obliquely incident on relativistically moving uniaxial and isotropic plasma slabs.