高强度均匀静磁场中氢原子能级的计算

采用一种简便的变分法,计算了在均匀高强度静磁场下氢原子的１１个低能态能级和平均半径,讨论了高强度磁场对能级和半径的影响。     

均匀磁场中氢原子低能级简并度的解除

讨论了均匀强磁场中氢原子哈密顿量中B^2项的影响,指出在忽略自旋－轨道相互作用的情况下,该项可使氢原子低能级简并度完全解除。     

同向电磁场中氢原子低能级简并的解除

利用同向电磁场的作用使氢原子低能级简并完全解除.     

均匀磁场中三维各向同性谐振子微扰矩阵元的普遍表达式

根据Laguerre多项式的积分公式,在考虑了哈密顿量中正比于B~2项影响的情况下,导出了均匀磁场中三维各向同性谐振子微扰矩阵元的普遍表达式,并指出n=3能级的简并度完全解除．     

利用均匀静磁场偏转带电粒子

本文叙述了在真空靶室中探测中性射线时在混合辐射条件下，为有效地偏转各种带电粒了，以消除其本底，提高测试的可信度，采用了均匀静磁偏转手段，效果很好。     

各种强度均匀磁场下氢原子定态问题统一求解

以简明的方式统一处理了塞曼效应，反常塞曼效应，帕邢－巴克效应以及中间强度均匀磁场下氢原子谱线的分分裂，移动和强度计算等问题。     

弱磁场中力矩的测定

用电子天平对均匀弱磁场中载流圆线圈所受力矩进行测量。     

同向电场磁场中氢原子的能级分裂

用通用软件Mathematica和简并微扰论计算了氢原子n=3~7能态在一对同方向电磁场中的能级分裂(不考虑自旋).数值结果表明:在许多情况下,一级修正可以使能级简并完全解除,这时总体能级分裂不是等间距的;但在一定条件下,总体能级分裂是等间距的,此时能级简并不能完全解除,只分裂为3n-2个不同能级.现有文章的结论是欠周全的.     

弱光场中氢原子的稳定性

虑一个处在弱光场中的经典氢原子系统,运用直接微扰方法求出了该系统微扰解的一般形式,并给出了解有界的条件。分析结果表明,在一般情况下,氢原子的微扰解是无界的,因而系统是Lyapunov不稳定的,但在解有界的条件满足时,系统则是Lyapunov稳定的。     

球形线圈磁场均匀性的研究

研究非密绕球形线圈内部的磁场均匀性质.从圆形电流线圈轴线上的磁场出发,利用叠加原理和Mathematica软件的计算和符号推导功能,得到一个关于线圈内部磁场均匀性与其匝数的定量关系式,在此基础上通过实例说明设计球形线圈磁场均匀区的方法.     

Photoelectric Effect on a Hydrogen Atom in an Extremely Strong Magnetic Field

Russian Physics Journal - The photoelectric effect on a hydrogen atom located in an extremely strong magnetic field is considered. The dependence of the cross section on the angle between the...     

Theoretical Calculation of Energy Levels of a Hydrogen Atom in a Strong Magnetic Field

The eleven low-lying energy levels of a hydrogen atom, and its mean radius in a uniformly high magnetic field B are calculated in a simple variational approach. The potential term containing squared magnetic field in Hamiltonian operator is separated into spherically and nonspherically symmetric potentials. The influence over levels and radius of the hydrogen atom is discussed. The results are in good agreement with the recent literatures, but more accurate. We find that the stronger the'magnetic field is, the smaller the mean radius of the hydrogen atom is.     

Quantum Deformation of the Two-Dimensional Hydrogen Atom in a Magnetic Field

The deformed Schrodinger equation for thetwo-dimensional hydrogen atom in a homogeneous magneticfield is obtained. It is found that the deformedpotential belongs to a new set of quasi-exactly solvable potentials.     

Absorption and Recurrence Spectra of Sodium Rydberg Atom in a Strong External Magnetic Field

Using core-scattered closed-orbit theory, we calculate the photoabsorption and the scaled recurrence spectra of sodium Rydberg atom in strong magnetic field below ionization threshold. The non-Coulombic nature of the ionic core have been modified by a model potential, which includes an attractive Coulomb potential and a short-ranged core potential. A family of core-scattered nonhydrogenic closed orbits have also been discovered. The Fourier transformed spectra of sodium atom have allowed direct comparison between peaks in such plot and the scaled action values of closed orbits. The new peaks in the recurrence spectra of sodium atom have been considered as effects caused by the core scattering of returning waves at the ionic core. The results are compared with those of hydrogen case, which show that the core-scattered effects play an important role in alkali-metal atoms.     

Berry's Phases of the Alkali Atom in a SlowlyChanging Strong Magnetic Field and Non-Adiabatic Transition

In this paper the high-order adiabatic approximation (HOAA) method is formulated in a new form ko that the calculation is greatly simplified. using this improved HOAA method, we study the Berry phase effects of the Alkali atom in a slowly-changing strong magnetic field and also the non-adiabatic transitions between the instantaneous angular momentum states. The possible observability is also pointed out.     

Accurate One-Centre Method for Hydrogen Molecule Ions in Strong Magnetic Field

An accurate one-centre method for the hydrogen molecule ion is tested. The slow convergence and singularities at the nuclear positions that are problems in the general one-centre method axe solved well by employing the optimal radial and angular B-spline basis. Therefore, the accuracy of the one-centre method is improved observably. For the ground state of the H2^＋ in the free field, 7 ×10^-8 accuracy is obtained, which rivals the best one-centre calculation before. As a test, the nuclear distances and the total energies of the 1σ g,u, 1πu, 1δ9,u and 2σg states of the H2^＋ for the magnetic field strength B = 1 a.u. are also obtained. Compared to other results, five-digit accuracy at least can be arrived even for the antibonding states 1σu and 1σu, whose equilibrium distances R is very large.     

Dynamics of a Rydberg Hydrogen Atom in a Generalized van der Waals Potential and a Magnetic Field

The classical dynamics of a Rydberg hydrogen atom in a generalized van der Waals potential plus a magnetic field is investigated by using the Poincaré surface of section and phase space trajectories method. The dynamical character of this system depends sensitively on the magnetic field strength. The numerical calculations show that for a certain van der Waals potential, its classical dynamics is regular without the external magnetic field. However, with the addition of the external magnetic field, the dynamical property of the Rydberg hydrogen atom begins to change. With the increase of the magnetic field strength, order-chaos-order-chaos types of transition regions are observed for the hydrogen atom. As the magnetic field strength is very large, nearly all the phase space trajectories are chaotic. Under this condition, only chaotic motion appears. This is caused by the diamagnetic Zeeman effect. Our study provides a different perspective on the dynamical behavior of the Rydberg atom in the van der Waals potential and magnetic field.     

Viscosity of a Magnetic Fluid in a Strong Magnetic Field

Acoustical Physics - The paper presents an estimate for the viscosity and its increment (“magneto-viscous” effect) in a thin wall layer of a magnetic fluid column oscillating in a tube...