金属氢的高压合成机理

 从氢原子间及氢分子间的相互作用入手，提出了固体氢中氢分子在高压作用下解离为氢原子，并以氢原子相互结合成金属氢的微观转化过程的机理。用这样的转化机理，可以解释毛河光等关于固体氢的拉曼光谱频率随高压变化规律的实验结果。     

二维氢原子径向方程的两种解法

本文利用两种方法求解二维氢原子的径向方程：一是升降算符法，由所定义的关于量子数ｍ的升降算符，给出了径向波函数之间的递推公式，求出了二维氢原子的能级和径向波函数的表达式；二是通过与三维氢原子径向方程的类比，在三维氢原子径向波函数的基础上，直接给出了二维氢原子径向波函数的一般表示式．两种解法所得结果完全一致．     

等效介质理论在氢—金属系统中的应用

近十年来发展起来的等效介质理论（ＥＭＴ），可以定性地，甚至在许多情况下可以定理地说明氢－金属系统的现象和特性，例如氢在金属表面上的化学吸附，金属中间隙氢原子的溶解热，金属缺陷对氢原子的俘获与排斥，金属中氢原子之间的相互作用，氢原子在金属中的扩散位垒等等．本文很据该理论及其和实验的比较，讨论了氢原子与金属之间的相互作用和有关现象．     

一维、二维、三维氢原子能级和电子分布概率

通过一维、二维氢原子定态薛定谔方程的严格解得出的能级公式和波函数，分析了一维、二维氢原子能级特点、简并度和电子分布概率，并将它们与三维氢原子进行比较，发现一维、二维、三维氢原子能级和电子分布概率有许多不同之处。     

EACVD中用氢原子谱线测定电子平均能量

采用蒙特卡罗方法，对EACVD中氢原子的发射过程进行了模拟。给出了由氢原子谱线测定电子平均能量的方法，结果对EACVD生长金刚石薄膜过程中实时监测电子平均能量，进而可以有效地控制工艺条件，生长出高质量的金刚石薄膜具有重要意义。     

光电子离开氢术核的方向

基态氢原子在电磁波的作用下发生电离，这主不是氢原子的光电效应，本文讨论氢原子的电子离开氢核的方向与电磁波的电场强度Ｅ的方向之间的关系。     

强激光场中模型氢原子和真实氢原子的高次谐波与电离特性研究

利用数值方法求解含时薛定谔方程，研究了一维、二维模型氢原子和真实的三维氢原子在强激光场中产生的高次谐波和电离特性.结果表明，在多光子电离区域和过垒电离区域，模型氢原子与真实的氢原子产生的高次谐波和电离概率差别很小；在隧道电离区域，它们产生的高次谐波的平台特征和截止位置相似，电离概率随时间变化的趋势相近，但其数值有明显的差异.对产生这种差异的原因进行了分析. 关键词： 强激光场 高次谐波 电离概率     

超强激光场中氢原子辐射高次谐波蒙特卡罗模拟

运用蒙特卡罗方法，模拟和计算出在超强激光场中，氢原子在相对论领域的电离几率和辐射出的高次谐波，并且讨论了氢原子的电离几率和辐射出的高次谐波与激光场的电场和磁场的关系。     

氢原子相干态研究的进展与启示

近年来的理论及实验研究都表明，在实空间中，期望用氢原子定态波函数的叠加以得到满足最小测不准关系的同时又不发生扩散的相干态是不可能的但若把三维氢原子体系映射到另外的空间，则可以发现氢原子体系可以存在真正的相干态，可这种相干态都不随物理的时间而是随另一个“虚假的时间”因子而演化。     

氢原子能级相对论修正的微扰方法的发散困难及其克服

指出现今所用的氢原子能级相对论效应微扰方法中蕴含着严重的发散困难，利用根式算符和动量表象克服了这种困难，重新计算氢原子各状态能级的相对论修正，并找到了前时结果在数值上所以正确的原因。     

Energy losses of a charged particle in a plasma in the presence of a strong electric field as a function of the sign of the charge

Institute of Radiophysics and Electronics, Academy of Sciences of the Armenian SSR. Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Radiofizika, Vol. 34, No. 4, pp. 347–351, April, 1991.     

On the asymmetry of a random walk in the presence of a field

Any ensemble of random walks with symmetric transition probabilities will have symmetric properties. However, any single realization of such a random walk may be asymmetric. In an earlier paper, Weiss and Weissman developed a measure of asymmetry and applied it to random walks in the absence of a field, showing that the degree of asymmetry (in the diffusion limit) is independent of time and that the most probable degree of asymmetry corresponds to the maximum possible. We show in the present paper how the presence of a symmetric field can change this result, both in making the degree of asymmetry depend on time, and driving the random walk toward a more symmetric state.     

Influence of the Porosity of the Surface of a Graphite Furnace on the Atomization of a Sample

The influence of the wear of a tube graphite furnace and the morphological features of its surface on the formation of an atomic-absorption signal has been investigated. Electron-microscopic and mass-spectrometric investigations have shown that, prior to atomization, copper in the form of elementary metal microparticles is found not only on the surface of the furnace but also in the bulk of its pores. Free atoms are formed as a result of the concurrent processes of atomization of a sample on the surface of the furnace and in the bulk of its pores. The change in the apparent energy of formation of free atoms of metals interacting actively with graphite in the process of atomization and the inflection on their Arrhenius plot have been explained qualitatively.     

On the dynamics of a particle on a cone

A detailed study of the classical and quantum mechanics of a free particle on a double cone and a particle bound to its tip by a harmonic oscillator potential is presented.     

On the dynamics of a particle on a hyperboloid

A free particle moving on a one-sheeted hyperboloid is discussed both at the classical and quantum levels.     

Effect of the field of a nonlinear electromagnetic wave on the shape of a soliton in a semiconductor superlattice

The effect of the electric component of the field of a high-frequency (HF) nonlinear electromagnetic (EM) wave on the propagation of a solitary EM wave (soliton) in a quantum semiconductor superlattice is studied. It is noted that in the collisionless approximation, the solution of the modified sine-Gordon equation corresponding to the amplification of an EM pulse that, with allowance made for interminiband electron transitions, transforms into a dissipative soliton is possible. The effect of electron collisions with irregularities of the crystal lattice on the soliton dynamics under the action of the field of a HF nonlinear wave is considered. The condition for an increase in the traveling time of the solitary wave is found.