多层周期薄膜中静磁表面波宽度模色散特性研究

首先建立了有限宽度、具有任意参数的多层薄膜结构中的静磁表面波（MSSW）宽度模普适色散方程,这一理论包含了利用多层薄膜控制静磁表面波色散特性的所有情形,使研究更加符合实际.对多周期的[(YIG/GGG)₁₀/金属层]多层膜结构窄样品中MSSW宽度模色散特性进行了数值计算,MSSW在多层窄样品中的工作主模为一阶宽度模式,多层膜的周期及参数可以有效地控制MSSW的色散特性,样品宽度效应也会对色散特性产生影响. 关键词：     

不均匀磁化薄膜中静磁波对导波光的Bragg衍射

研究了横向不均匀偏置磁场作用下掺Bi的YIG薄膜中微波静磁波的激发和传播特性;采用变分方法计算了静磁正向体波的色散关系和交变磁化强度,分析了不均匀场对静磁波－导波光耦合的影响理论计算得到的衍射效率曲线与实验结果基本一致,表明适当不均匀场可以大大提高磁光Bragg器件的衍射性能.     

基于两种静磁模的磁光压缩特性比较

将磁光效应作为微扰, 采用耦合模理论分析了磁光薄膜波导中微波静磁波对线性啁啾光脉冲的磁光Bragg衍射作用, 得到了传统磁化时磁光共线和非共线作用下的衍射光脉冲复振幅的解析表达式。在静磁波频率和波数相同的前提下, 通过对实际波导结构的计算表明, 基于静磁表面波的磁光共线作用比基于静磁正向体波的非共线作用更易于实现光脉冲压缩; 衍射光脉冲的半极大全宽度(FWHM)对失配斜率的依赖较为敏感。因此, 选用磁光共线作用和优化相位失配因子的频率变化率有助于改善磁光Bragg脉冲压缩器的性能。     

GdFeCo/AlN/TbFeCo薄膜的变温磁化性能研究

用磁控溅射法制备了GdFeCo/AlN/TbFeCo静磁耦合多层薄膜。振动样品磁强计和克尔磁滞回线测试装置的测试结果表明 :2 5℃不加外磁场时GdFeCo/AlN/TbFeCo静磁耦合多层薄膜读出层 (GdFeCo)的极向克尔角为零 ,读出层呈平面磁化 ;12 5℃不加外场时读出层的克尔角最大 (0 .5 4°) ,读出层的磁化方向为垂直磁化 ;随着温度增高 ,读出层由平面磁化转变为垂直磁化 ,在 75℃到 12 5℃温度范围内读出层磁化方向很快从平面磁化转变为垂直磁化。对磁化过程的机理研究表明 :饱和磁化强度和有效各向异性常量影响读出层磁化方向的转变过程 ,但主要受读出层饱和磁化强度的影响 ;在较高温度时读出层的磁化强度较小 ,退磁场能较小 ,在静磁耦合作用下 ,使GdFeCo读出层的磁化方向发生转变。制备的GdFeCo/AlN/TbFeCo静磁耦合多层薄膜适合作CAD MSR记录介质     

非线性静磁表面波的传播特性

将文献[4]的理论结果加以推广,用微扰理论导出了微波场作用下铁磁材料的动态非线性磁化强度的各阶近似表达式。严格分析了在波矢k与外偏置磁场H₀成任意角度时非线性静磁表面波的传播特性。证明了静磁表面波在任何传播方向上都不能演化为静磁孤子。 关键词：     

GdFeCo/AIN/TbFeCo薄膜的变温磁化性能研究

用磁控溅射法制备了GdFeCo/AlN/TbFeCo静磁耦合多层薄膜.振动样品磁强计和克尔磁滞回线测试装置的测试结果表明:25℃不加外磁场时GdFeCo/AlN/TbFeCo静磁耦合多层薄膜读出层(GdFeCo)的极向克尔角为零,读出层呈平面磁化;125℃不加外场时读出层的克尔角最大(O.54°),读出层的磁化方向为垂直磁化;随着温度增高,读出层由平面磁化转变为垂直磁化,在75℃到125℃温度范围内读出层磁化方向很快从平面磁化转变为垂直磁化.对磁化过程的机理研究表明:饱和磁化强度和有效各向异性常量影响读出层磁化方向的转变过程,但主要受读出层饱和磁化强度的影响;在较高温度时读出层的磁化强度较小,退磁场能较小,在静磁耦合作用下,使GdFeCo读出层的磁化方向发生转变.制备的GdFeCo/AlN/TbFeCo静磁耦合多层薄膜适合作CAD-MSR记录介质.     

线偏振激光在磁化等离子体中的调制不稳定性

 采用洛伦兹变换推导了线性偏振激光在磁化等离子体中的非线性色散关系,根据Karpman方法推导出横波的非线性控制方程,利用线性偏振激光在磁化等离子体中的非线性色散关系和非线性控制性方程,分析了在磁化等离子体中有限振幅的扰动引起的调制不稳定性,得到了线性偏振激光的调制不稳定的时间增长率与扰动波数之间的函数关系。分析结果表明：激光等离子体的临界面附近的磁调制不稳定性的时间增长率显著增大。     

静磁表面波对高斯光脉冲的衍射特性研究

研究了磁光薄膜波导中线性啁啾高斯光脉冲与单频连续静磁波共线作用,给出了水平磁化时基于静磁表面波的磁光耦合方程.分别采用解析法和数值法计算了1310 nm和1550 nm两种光波长入射时衍射光的压缩特性,两种求解方法得到的结果一致.计算表明,衍射光脉冲的半峰全宽(FWHM)随相位失配因子的频率变化率和啁啾系数的增大而减小;在给定的计算参数下,与1310 nm波长对应的衍射光脉冲具有较大的峰值强度,但1550 nm波长输入时可以获得更窄的衍射光脉冲,因而1550 nm光脉冲更适于作为磁光脉冲压缩的脉冲源.文章还分析了磁损耗对衍射光脉冲的光强和输出脉宽的影响,对于普通的磁光薄膜,损耗基本上不影响光脉冲压缩效果.     

载流子影响下铁磁膜中静磁孤子的存在性分析

铁磁膜近邻存在半导体载流子的影响下,静磁表面波在一定频率范围内与外加恒磁场相垂直的传播方向上能演化成静磁孤子,而且静磁表面波群速在一定频率范围会改变运动方向成为反向波,其大小受载流子浓度的影响 关键词： 静磁孤子 载流子 铁磁膜 静磁表面波     

非线性传输线数值模拟方法

给出了模拟交叉耦合磁饱和非线性传输线的数值模拟方法,算法基于传输线各节点的时域差分方程组进行步进迭代,其中利用J-A模型描述传输线中铁氧体磁芯的非线性磁化行为。根据节点电路方程推导了非线性传输线色散关系,设计了输出频率为300 MHz的交叉耦合磁饱和非线性传输线,利用本数值模拟方法对交叉耦合磁饱和非线性传输线的物理过程进行了分析,在充电电压达到30kV时获得了频率303MHz、峰峰值不小于40kV的高压射频脉冲输出。     

Nonlinear Dispersion of Magnetostatic Surface Waves on Ferromagnetic Films

The wave equation of nonlinear magnetostatic surface waves (MSSW) on ferromagnetic films is derived and its solution is found. The nonlinear dispersion relation of MSSW in discussed. Our Result shows that the wave power has a little effect to the frequency shift of MSSW with lower frequency, but has a considerably larger effect to that with higher frequency within the band.     

A granular high-temperature superconductive film in the field of a magnetostatic surface wave

The reflection of a magnetostatic surface wave from a strip of a granular high-temperature superconductor is investigated. An expression obtained by the method of perturbations describes the field of the scattered wave. The coefficient of reflection of the MSSW from the HTSC strip is calculated as a function of frequency and temperature. It is shown that the reflectance is very low at temperatures above critical and that the HTSC ceramic behaves as an ordinary superconductor. The reflectance rises sharply when the temperature drops below critical. As the critical current decreases, the reflectance drops off and the film loses the high-temperature properties. An expression is derived for the loss resistance of the MSSW in a granular HTSC film. The loss resistance amounts to a few kiloohms and falls off sharply as the film transitions to the superconductive state. The results can also be developed for periodic HTSC structures and used in the design of frequency-selective devices, as well as high-speed bolometric photodetectors. Tomsk State University of Control Systems and Electronics. Translated Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 7, pp. 97–102, July, 1998.     

Four-magnon decay of magnetostatic surface waves in yttrium iron garnet films

The four-magnon instability of magnetostatic surface waves (MSSWs) in yttrium iron garnet epitaxial films is investigated experimentally. It is shown that four-magnon instability for MSSWs with wave numbers 30–600 cm⁻¹ is a decay instability and develops for values of the wave magnetization close to the threshold level for second-order parametric instability of a homogeneous transverse pump wave. When the supercriticality of the MSSW power is 15–20 dB, the generated parametric spin waves themselves become unstable with respect to the four-magnon interaction, so that kinetic instability develops in the film. It is shown that the pump signal transmitted through the signal and the length of the “nonlinear” part of the film, where a MSSW is capable of exciting parametric spin waves, increase as the pump power is increased. Fiz. Tverd. Tela (St. Petersburg) 38, 330–338 (February 1997)     

Surface wave propagation at the interface between lossy metamaterials medium and nonlinear media with arbitrary nonlinearity

The dispersion relation in a system that consists of a lossy metamaterials (MTMs) film surrounded by a linear substrate and a nonlinear cladding with an arbitrary nonlinearity is derived. The surface plasmonic (SP) wave at the interfaces between metamaterials (MTMs) and the nonlinear cover is recovered by taking certain limits. Lossy MTMs have simultaneously complex-negative permeability μ and complex-negative permittivity ε. Results are presented by plotting the SP frequency as a function of the nonlinearity at chosen damping factors. Both the real and imaginary parts are studied. Results also display the wave frequency as a function of plasma frequency. For comparison, the imaginary part is set to zero and curves are reproduced.     

Nonlinear planar optical waveguide sensors comprising metamaterial guiding films at terahertz frequencies

In this paper, we propose a metamaterial film bounded by a nonlinear cover and a dielectric substrate as a THz wave sensor. The dispersion characteristics and magnetic field profiles have been derived, computed and analyzed. Confinement of the light waves was found to increase with both nonlinearity and frequency. We believe our results can be used to design novel tunable future sensors.     

Solution to the influence of the MSSW propagating velocity on the bandwidths of the single-scale wavelet-transform processor using MSSW device

The objective of this research was to investigate the possibility of solving the influence of the magnetostatic surface wave (MSSW) propagating velocity on the bandwidths of the single-scale wavelet transform processor using MSSW device. The motivation for this work was prompted by the processor that −3 dB bandwidth varies as the propagating velocity of MSSW changes.In this paper, we present the influence of the magnetostatic surface wave (MSSW) propagating velocity on the bandwidths as the key problem of the single-scale wavelet transform processor using MSSW device. The solution to the problem is achieved in this study. we derived the function between the propagating velocity of MSSW and the −3 dB bandwidth, so we know from the function that −3 dB bandwidth of the single-scale wavelet transform processor using MSSW device varies as the propagating velocity of MSSW changes. Through adjusting the distance and orientation of the permanent magnet, we can implement the control of the MSSW propagating velocity, so that the influence of the MSSW propagating velocity on the bandwidths of the single-scale wavelet transform processor using MSSW device is solved.     

Nonlinear wave propagation along periodic-loaded transmission line

A high frequency transmission line periodically loaded with varactor diodes is presented to study nonlinear wave propagation. The nonlinearity and dispersion characteristics are experimentally and theoretically analysed. Experimental results on shock wave formation and harmonic frequency generation are found to be in good agreement with theoretical predictions. The influence of dispersion on second-harmonic frequency generation is particularly discussed yielding large values of the efficiency.     

The effect of the nonparabolicity of the free carriers dispersion law on the propagation of surface polaritons in a semiconductor-metal structure

The results of a study on the influence of the nonparabolicity of the free carriers dispersion law on the propagation of surface polaritons (SPs) located near the interface between an n-type semiconductor and a metal arc reported. The semiconductor plasma is assumed to be warm and nonisothermal. The nonparabolicity of the electron dispersion law has two effects. The first one is associated with nonlinear self-interaction of the SPs. The nonlinear dispersion equation and the nonlinear Schrodinger equation for the amplitude of the SP envelope are obtained. The nonlinear evolution of the SP is studied on the base of the above mentioned equations. The second effect results in third harmonics generation. Analysis shows that these third harmonics may appear as a pure surface polariton, a pseudosurface polariton, or a superposition of a volume wave and a SP depending on the wave frequency, electron density and lattice dielectric constant.     

Optical second-harmonic generation in a thin-film waveguide without control of film thickness

An optical second-harmonic wave can be generated in a three-layered optical waveguide of arbitrary film thickness under phase-matching condition. Phase-matching is achieved by utilizing mode dispersion in an optical waveguide with a two-dimensional configuration. A numerical analysis of the matching condition is given and the results of the observation of the optical second-harmonic wave of a guided Nd : YAG laser in a Ti-indiffused LiNbO₃ nonlinear film are described.