ν↓型三能级原子系统中Raman跃迁增强的Kerr非线性效应

在理论上研究了ν↓型三能级原子系统Raman跃迁中的线性和非线性极化率．研究表明：Raman跃迁中，如果原子完全被抽运到与控制光作用的基态时，将导致介质对探针光的线性极化率为零，而三阶非线性极化率不为零．通过减小原子两基态间的无辐射衰减速率γ12，可以极大地增强交叉Kerr非线性效应．     

极化电子与原子散射的广义Stokes参量的实验测量

分析了极化电子与原子散射后的受激原子退激辐射光的广义Stokes参量，介绍了Stokes参量的基本概念和实验测量方法并阐明其具体的物理意义．为自旋极化电子参与的原子或分子碰撞实验和理论模型的研究奠定基础．     

光泵原子磁力仪及其应用

光泵原子磁力仪是利用激光极化原子气体,外磁场与原子相互作用使原子光学性质发生变化,进而改变探测光的偏振方向或光强。原子磁力仪精度已超过超导磁力仪,但是体积重量比超导磁力仪小。给出了碰撞混合以及驰豫与极化速率以及最终极化度的定量关系,总结了原子磁力仪国内外研究进展以及在导航领域的应用。     

原子实极化效应和钠原子s系列高Rydberg态能级寿命的计算

利用相关效应的模型势方法计算了钠原子Rydberg态s系列的能级寿命.此理论方法不依赖于实验参数.计算结果很好地符合实验值，并证实了这一理论模型的合理性. 关键词： 原子实极化 Rydberg态 跃迁矩阵元 辐射寿命     

慢电子与He和Ne原子弹性碰撞的极化作用及散射截面计算

本文对慢电子与原子碰撞的一种常用的极化势模型进行了修正，使其在近区描述的入射电子使靶原子的极化作用更符合实际。用此修正后的极化势，在０．２－３０ｅＶ能量范围内，本文还计算了电子被Ｈｅ和Ｎｅ原子弹性散射的总截面和微分散射截面。结果有很大改进，与实验符合得较好，说明本文的极化势修正是合理的。     

静电场中电介质的极化能

本文通过处于理想平板电容器中的一种电介质原子的极化模型，在经典物理范围内讨论了与电介质中静电场能量有关的问题．特别是关于静电场中电介质的极化能，说明它作为介质中静电场能量的组成部分在微观上的意义．     

单镜面附近激发态极化原子的自发辐射简

利用格林函数和费米黄金定律,我们计算了单镜面附近的激发态极化原子的自发辐射率.结果表明:原子的自发辐射与原子的极化偶极距取向有关,并且随着原子与镜面间距的增大,辐射率呈现正弦形式的振荡.当偶极距取向与镜面方向平行时,自发辐射的正弦式振荡最为激烈.但是随着极化方向与镜面方向夹角的增大,自发辐射的振荡越来越弱.当偶极距取向与镜面垂直时,振荡几乎消失.利用光子的闭合轨道理论,我们可以发现激发态原子偶极距取向影响辐射光子数的多少,从而可以改变原子的自发辐射率.     

单镜面附近激发态极化原子的自发辐射

利用格林函数和费米黄金定律,我们计算了单镜面附近的激发态极化原子的自发辐射率。结果表明：原子的自发辐射与原子的极化偶极距取向有关,并且随着原子与镜面间距的增大,辐射率呈现正弦形式的振荡。当偶极距取向与镜面方向平行时,自发辐射的正弦式振荡最为激烈。但是随着极化方向与镜面方向夹角的增大,自发辐射的振荡越来越弱。当偶极距取向与镜面垂直时,振荡几乎消失。利用光子的闭合轨道理论,我们可以发现激发态原子偶极距取向影响辐射光子数的多少,从而可以改变原子的自发辐射率。     

Λ型三能级原子系统中Raman跃迁增强的Kerr非线性效应

在理论上研究了Λ型三能级原子系统Raman跃迁中的线性和非线性极化率.研究表明: Raman 跃迁中，如果原子完全被抽运到与控制光作用的基态时，将导致介质对探针光的线性极化率 为零，而三阶非线性极化率不为零.通过减小原子两基态间的无辐射衰减速率γ_{12，可以极大地增强交叉Kerr非线性效应.}     

钾原子基态的定量证明

用原子实模型简化钾原子的哈密顿,把原子实极化和轨道贯穿视为微扰,用微扰法计算了钾原子的能量,定量证明了钾原子的基态是4s态．     

石墨烯等二维原子晶体薄片样品的光学衬度计算及其层数表征

本文以鉴别机械剥离法制备的高质量石墨烯样品的层数为例, 阐明了如何利用传输矩阵来计算二维原子晶体薄片样品的光学衬度, 并进一步精确地鉴别其层数. 计算结果表明测试时所选用的显微物镜数值孔径对精确确定薄片样品的层数非常重要, 并为实验所证实. 同时提出了使用两个激光波长可以快速地表征样品尺寸接近物镜衍射极限的薄片样品层数的方法. 本文所采用的传输矩阵形式非常适合于计算二维原子晶体薄片样品的光学衬度, 并可以方便地推广到更复杂的多层衬底结构, 以便快速和准确地鉴别各种衬底上二维原子晶体薄片样品的厚度. 关键词： 二维原子晶体材料 层数 传输矩阵 光学衬度     

Structural examination of lithium niobate ferroelectric crystals by combining scanning electron microscopy and atomic force microscopy

The structure of lithium niobate single crystals is studied by a complex technique that combines scanning electron microscopy and atomic force microscopy. By implementing the piezoresponse force method on an atomic force microscope, the domain structure of lithium niobate crystals, which was not revealed without electron beam irradiation, is visualized     

Suppression and Acceleration Effects of Measurements on A-type Atomic Decay in Anisotropic Photonic Crystals

The measurement-induced suppression and acceleration effects on A-type atomic decay in three-dimensional anisotropic photonic crystals are investigated. We consider the two cases, only one or both of the two atomic resonant frequencies being near the band edge of a photonic crystal. Due to the deformation of the electromagnetic density of states, the repeated projection onto the excited state can lead to decay suppression or acceleration effect already at rather low repetition rates. Such measurement-induced effects are dependent on the frequency of measurements and the relative position of the atomic upper level from the band edge of photonic crystals. The behaviors of instant and effective decay rates are studied in detail, which are different from the case of isotropic photonic crystals.     

Nonlinear Gap Modes in a 1D Alternating Bond Monatomic Lattice with Anharmonicity

We analytically study the nonlinear localized gap modes in a one-dimensional atomic chain with uniform atomic mass but two periodically alternating force constants between the nearest neighbors by means of a quasi-continuum approximation. This model simulates a row of atoms in the <111> direction of a diamond-structure type of crystals or molecular crystals with alternating double and single bonds. For this lattice system, we find that the harmonic plus quartic anharmonic terms of inter-site potential produce a new type of nonlinear localized gap modes with a slightly asymmetry distribution of atomic displacements. These localized gap modes are somewhat different from widely studied localized gap modes with a symmetry atomic displacement distribution in diatomic ion lattices.     

Magnetosensitive intermediate states of point-defect complexes formed as a result of quenching of NaCl: Eu single crystals

A correlation between temporal variation in the optical and mechanical properties of quenched NaCl: Eu single crystals and the sensitivity of these crystals to a constant magnetic field was found. The results obtained make it possible to assess the atomic structure of magnetosensitive point-defect complexes.     

Ferromagnetic films with magnon bandgap periodic structures: Magnon crystals

A new type of photonic crystals is proposed. The new crystals have a forbidden gap in the microwave spectrum of magnetostatic spin waves, and, by analogy with photonic crystals, they are called magnon crystals. Specimens of such crystals were fabricated on the basis of yttrium iron garnet films. The surfaces of ferromagnetic films containing two-dimensional etched hole structures were studied by atomic force and magnetic force mag-netometry. The propagation of spin waves through the magnon crystals was investigated.     

Spectral anisotropy of a photoresponse from heterojunctions based on GaSe and InSe layered crystals

The object of investigation is photoresponse spectra taken from the cleaved end face of heterojunctions formed by GaSe and InSe anisotropic crystals. Spectra taken from the as-prepared and chemically processed faces of the heterojunctions are compared. A modified method of growing GaSe crystals with a virgin end face is suggested, and the surface of GaSe crystals thus grown is examined by atomic force microscopy.     

Multicrystal microundulator

The mode of propagation of relativistic, positively charged particles through a system of mutually oriented and periodically arranged ultrathin crystals whose thicknesses are equal to the half-period of the particle trajectory during planar channeling in a thick crystal is considered. In the case of an incidence angle that is less than the critical channeling angle, a certain fraction of particles is specularly reflected from the atomic planes of the crystal. Therefore, passing through a stack of crystals, a particle moves along quasiundulator trajectories. The characteristics of the radiation of a particle passing through such a “multicrystal microundulator” are found. The radiation spectrum is discrete, and the first-harmonic frequency and the number of harmonics in the spectrum are dependent on the distance between the crystals, the particle energy, and the potential of atomic planes of the crystal. Radiation is concentrated in a narrow cone in the direction of the average velocity of particles and is mainly polarized in a plane that is orthogonal to the atomic planes of the crystal. The microundulator can be composed of separate crystals with micron thicknesses and can be fabricated using modern methods of microlithography and micromechanics with deep, for example, plasmochemical etching of the crystal surface.     

Optical contrast of a photonic crystal and the self energy shift of the energy levels of atoms

The influence of a photonic crystal medium on the character of the interaction of electrons with their own radiation field is studied. As was recently shown, this influence changes the electromagnetic mass of the electrons in photonic crystals. This alters atomic energy levels. The dependence of this effect on the optical contrast of photonic crystals is studied.     

Negative longitudinal expansion and the amplitude of longitudinal vibrations in poly(ethylene) crystals

The experimental temperature dependences of the thermal expansion coefficient and the mean-square amplitude of atomic vibrations in the longitudinal direction (along the axes of chain molecules) in poly(ethylene) crystals of different sizes are measured using x-ray diffraction in the temperature range 5–350 K. Theoretical calculations of the temperature dependences of the thermal expansion coefficient and the mean-square amplitude of atomic vibrations in poly(ethylene) crystals are carried out. It is shown that the results of calculations are in good agreement with experimental data. The temperature ranges in which the quantum character of lattice dynamics affects the thermal expansion coefficient and the mean-square amplitude of vibrations are determined. It is revealed that the shear longitudinal modes play an important role in the lattice dynamics of crystals with a chain structure.