薄膜物理及其应用讲座第五讲Fe－Si／X（Si，Cu，Pd，Cr）多层膜的磁性研究

系统研究了由非晶态Ｆｅ－Ｓｉ合金与Ｓｉ，Ｃｕ，Ｐｄ和Ｃｒ四种不同类型的材料组合而成的磁性多层膜的二维磁性，界面的死层效应和极化效应，层间耦合作用。在Ｆｅ－Ｓｉ／Ｃｒ多层膜研究中，发现了饱和磁化强度随Ｃｒ层厚度的改变而出现振荡变化的现象，这是由于磁性层甲内场的变化，特别是顺磁分量发生振荡变化引起的。     

薄膜物理及其应用讲座：第五讲 Fe—Si／X（Si,Cu,Pd,Cr）多层膜的磁性研究

系统研究了由非晶态Ｆｅ－Ｓｉ合金与Ｓｉ、Ｃｕ，、Ｐｄ和Ｃｒ四种不同类型的材料组合而成的磁性多层膜的二维磁性，界面的死层效应和极化效应，层间耦合作用，在Ｆｅ－Ｓｉ／Ｃｒ多层膜研究中，发现了饱和磁化强度随Ｃｒ层厚度的改变而出现振荡变化的现象，这是由于磁性层中内地场的变化，特别是顺磁分量发生振荡变化引起的。     

半花菁LB多层膜的光致各向异性研究

用光学线性和非线性方法研究了Ｙ型半花菁／花生酸交替ＬＢ多层膜的光致光学各向异性。在纳秒紫外偏振脉冲激光照射下，ＬＢ多层膜中半花菁分子发色团长轴向紫外光偏振方向重新取向。加热可以使ＬＢ多层膜平面内各向异性消失及Ｈ－聚集体分解。     

周期性起伏四层磁性薄膜的克尔效应

结合干涉光刻和磁控溅射制备了一维周期性起伏的磁性多层薄膜。利用扫描探针显微镜对样品的微结构进行表征,利用椭偏仪和磁光测量系统对样品的光学性能参数和磁光克尔效应进行测试和研究。实验结果发现,磁性多层薄膜磁光性能得到极大的提升,磁光增强的克尔谱峰值与条带的宽度、中间层二氧化铪层的厚度有关;利用介质层的厚度可调制复合薄膜的磁光特性。进一步研究发现横克尔效应的增强现象。理论计算的结果证实,磁光增强源于光学腔干涉共振和磁等离激元的耦合效应。     

利用P—偏振光双面反射法测量多层膜的光学参数

利用Ｐ－偏振光双面反射法测量了浸泡提拉法制备了“有机硅树脂－二氧化硅－有机硅树脂”三层膜样品两面Ｐ－偏振光反射强比γ与入射角θ关系曲线，经过数据拟合，确定了这三层薄膜的光学参数，同时研究了薄膜间的相互作用层的光学参数，测量结果表明此方法可能成为研究薄膜和膜层之间的相互作用的一种新手段。     

稀释磁性半导体

稀释磁性半导体是指Ⅱ－Ⅵ族、Ⅳ－Ⅵ族、Ⅱ－Ⅴ族或Ⅲ－Ⅴ族化合物中，由磁性过渡族金属离子或稀土金属离子部分地替代非磁性阳离子所形成的新的一类半导体材料。这类材料的突出特点是磁性离子磁矩和能带电子自旋之间存在交换相互作用。由此引起材料性质发生一系列重要变化。本文系统介绍这类材料的各种物理性质，包括能带结构，ｓｐ－ｄ和ｄ－ｄ交换作用，磁性质和自旋玻璃特性，光学和磁学性质，输运特性等。最后简单介绍这类材料     

可精密测定多层金属膜厚度的激光超声声呐

可精密测定多层金属膜厚度的激光超声声呐光学方法可以精密测定透明薄膜的厚度，如多角度、多波长椭偏仪可测量厚度小于３ｎｍ的氧化层、厚度大于１０μｍ的光刻胶以及氧化物－多晶硅等多层结构．但对不透明的多层金属膜的测量一直受到很大的限制．最近，ＲｕｄｏｌｐｈＴ...     

光电子学与光电子产业专题系列介绍：用于X射线光学的多层膜

用于Ｘ射线，特别是软Ｘ射线（波长范围约为３０－１ｎｍ）光学中的多层膜近十年来引起了人们的广泛重视，取得了许多重要进展．本文对这类多层膜的特点、制备和检测方法以及应用等作简要介绍．     

X射线布拉格-菲涅耳光学元件的实验研究

用光学全息方法在涂有光刻胶的多层膜表面上的形成布拉格－菲涅耳元件所需的波带片图形,通过离子束刻蚀方法将波带片图形转写到多层膜上,完成元件的制作,给出布拉格－菲涅耳光学元件测量结果,测量结果表明上述方法适于制作布拉格－菲涅耳元件。     

应用于光隔离器的一维磁光光子晶体结构探索

采用传输矩阵方法分析了一维磁光光子晶体.对不同结构参量下的磁光多层膜的光学性质进行了数值计算.得到了一种新颖实用的磁光多层膜结构,可用作实现光集成应用中的光隔离器的元件.典型磁光材料的厚度仅为2.13 μm,一维磁性光子晶体的总厚度仅为7.03 μm.     

磁场中准二维强耦合磁极化子的有效质量

采用改进的线性组合算符和LLP变分法,研究了外磁场对量子阱中电子与界面光学声子强耦合、与体纵光学声子弱耦合磁极化子的有效质量的影响。对AgCl/KI量子阱进行了数值计算,结果表明,磁极化子的有效质量随阱宽的增加而减小,随磁场的增强而增大,但不同支声子与电子和磁场相互作用对磁极化子有效质量的贡献大不相同。     

Interface Polaron Within Parallel Electric and Magnetic Fields

A combinative method of variational wavefunction and harmonic oscillator operator algebra is used to treat the interface polaron in a semi-infinite polar crystal within parallel electric and magnetic fields perpendicular to the interface. Both the bulk longitudinal optical phonon and the interface optical phonon together with the anisotropic mass of the electron are included. The energy level correction up to the second-order perturbation, cyclotron-resonance frequency and cyclotron mass are expressed as functions of the electric and magnetic fields and a parameter characterizing the mean distance of the polaron from the interface. This theory is used to calculate numerically the single heterostructure AlAs/GaAs, when the electron is at the X high-symmetry point of the conduction band of AlAs. The results show that the magnetic field greatly enhances the polaronic correction of the electron energy levels while the electric field only increases the correction of their surface optical phonon part but obviously decreases that of their bulk optical mode part and thus the total energy correction decreases as the electric field increases. The change of red shift due to the electron-phonon interaction with electric and magnetic fields is also obf ained.     

表面极化子光学声子平均数的磁场和温度依赖性

采用变分法、幺正变换和拉格朗日乘子法,研究了有限温度下纯二维晶体中表面磁极化子的性质.讨论了表面光学声子平均数、磁极化子振动频率λ与磁场B、温度T及Lsgrange乘子u之间的关系.对KCl晶体进行了数值计算,结果表明:磁极化子振动频率、表面光学声子平均数均随磁场B的增强而增加,且随温度T升高而增加.当bgrange乘子u超出慢电子范围时磁极化子振动频率、表面光学声子平均数均随u增加而增大且变化越来越显著.     

Optical Magnetic Mirror from the Viewpoint of Molecular Optics

Russian Physics Journal - A condition for realization of an optical magnetic mirror at the interface between the vacuum and the medium consisting of electric dipoles (or electric and magnetic...     

Cyclotron resonance of a polaron in a realistic heterojunction and its pressure effect

The Larsen perturbation method is adopted to study the influence of magnetic fields on polarons in realistic heterojunctions in a quasi-two-dimension approximation. The interaction between an electron and both the bulk longitudinal optical phonons and the two branches of interface optical phonons is taken into account to show the influence of magnetic fields at different ranges on the polaron cyclotron mass due to the coupling of the electron with each branch of phonon modes. The result indicates that not only do the bulk phonons influence the polaron cyclotron mass, but the interface phonons do as well. The pressure effect on the cyclotron mass is also discussed.     

High order matched interface and boundary methods for the Helmholtz equation in media with arbitrarily curved interfaces

This work overcomes the difficulty of the previous matched interface and boundary (MIB) method in dealing with interfaces with non-constant curvatures for optical waveguide analysis. This difficulty is essentially bypassed by avoiding the use of local cylindrical coordinates in the improved MIB method. Instead, novel jump conditions are derived along global Cartesian directions for the transverse magnetic field components. Effective interface treatments are proposed to rigorously impose jump conditions across arbitrarily curved interfaces based on a simple Cartesian grid. Even though each field component satisfies the scalar Helmholtz equation, the enforcement of jump conditions couples two transverse magnetic field components, so that the resulting MIB method is a full-vectorial approach for the modal analysis of optical waveguides. The numerical performance of the proposed MIB method is investigated by considering interface problems with both constant and general curvatures. The MIB method is shown to be able to deliver a fourth order of accuracy in all cases, even when a high frequency solution is involved.     

Dynamical behavior of coupled magnetic bilayers

We obtain the magnetic susceptibility of systems constituted of two coupled magnetic layers. We consider that the coupling of the films is well described by a Heisenberg like interaction to write the equation of motion for the magnetization of each part of the system. The dynamical response of each constituent material is calculated taking into account the presence of an interacting magnetic media (a magnetic layer) in its border. The susceptibility obtained incorporates the effects of a different magnetic film in the neighborhood (via the interfilm interaction), as well as the properties of the interface. We use a procedure similar to the effective medium approach developed for superlattices to obtain an effective magnetic permeability for the whole system. We show that the knowledge of this property allows one to have information on the interface of the magnetic bilayer through the analysis of its optical properties. We illustrate this point by calculating the dispersion relation of magnetic polaritons propagating in a system consisting of an antiferromagnetic (MnF₂) layer grown in direct contact with a ferromagnetic film (Fe). We also simulate numerically an optical experiment where ATR (Attenuated Total Reflection) spectra are obtained.     

Light switching at a prism-liquid crystal interface. A new sensor for magnetic fields

Light beam propagation at a prisms-liquid crystal interface is studied both theoretically and experimentally. Our results suggest the possibility of employing such an interface as an element while designing optical sensors for magnetic fields. A comparison between the data of a theoretical model based on the Berreman formalism and the experimental results is presented.     

Designing optical-fiber modulators by using magnetic fluids

To reduce interface loss between optical fibers and devices in telecommunication systems, the development of an optical-fiber-based device that can be fused directly with fibers is important. A novel optical modulator consisting of a bare fiber core surrounded by magnetic fluids instead of by a SiO2 cladding layer is proposed. Applying a magnetic field raises the refractive index of the magnetic fluid. Thus we can control the occurrence of total reflection at the interface between the fiber core and the magnetic fluid when light propagates along the fiber. As a result, the intensity of the outgoing light is modulated by variation in field strength. Details of the design, fabrication, and working properties of such a modulator are presented.     

Simulation of optically pumped intersubband laser in magnetic field

Simulations of an optically pumped intersubband laser in magnetic field up to 60 T are performed within the steady-state rate equations model. The electron-polar optical phonon scattering is calculated using the confined and interface phonon model. A strong oscillatory optical gain vs. magnetic field dependence is found, with two dominant gain peaks occurring at 20 and 40 T, the fields which bring appropriate states into resonance with optical phonons and thus open additional relaxation paths. The peak at 20 T exceeds the value of gain achieved at zero field.