环形非球谐振子径向矩阵元的通项公式及其递推关系

环形非球谐振子的势能函数为V(r,θ)=12mω2r2+22mAr2+22mbr2sin2θ,其精确的能谱方程和归一化的波函数已经获得.在此基础上,给出了环形非球谐振子径向矩阵元的通项公式和不同幂次径向矩阵元之间所满足的递推关系.作为特例,讨论了球谐振子、非球谐振子和环形振子的有关结果. 关键词： 环形非球谐振子 径向矩阵元 通项公式 递推关系     

各向同性谐振子径向矩阵元的通项表达式

推导出三维各向同性谐振子径向矩阵元p|n′l′>和二维各向同性谐振子径向矩阵元q|n′m′>的通项表达式- 关键词：     

相对论性氢原子径向算符矩阵元的通项计算公式

给出了相对论性氢原子径向算符矩阵元〈n′₁,K₁,j₁,m_j1|r^p|n′₂,K₂,j₂,m_j2〉的通项计算公式. 关键词：     

n维氢原子径向矩阵元的通项计算公式

给出了ｎ维氢原子的归一化径向波函数,推导出了ｎ维氢原子的任意径向矩阵元〈ＮＪ｜ｒ＾ｑ｜Ｎ′Ｊ′〉的通项计算公式。     

N维各向同性谐振子径向矩阵元的递推公式

各向同性谐振子是量子理论中能够严格求解的可解势场之一.对它的研究和讨论,在理论上和实际的应用中都有重要意义.本文推导出了N维(N≥2)各向同性谐振子径向矩阵元〈nrl|rk|nr′l′〉的递推公式,在此基础上得到了平均值的递推公式,并且讨论了维各向同性谐振子径向矩阵元的递推公式的一般性,而文献[3]与[4]所给出的各向同性谐振子径向矩阵元的递推公式只是本文结论的特例.     

m维氢原子径向矩阵元的通项计算公式

给出了n维氢原子的归一化径向波函数,推导出了n维氢原子的任意径向矩阵元〈NJ|rq|N′J′〉的通项计算公式。     

三维各向同性谐振子径向矩阵元的递推关系

推导出三维各向同性谐振子径向矩阵元〈nl|rp|n′l′〉所满足的递推关系 关键词：     

相对论性无自旋氢原子径向矩阵元的通项公式及平均值的解析表达式

给出了相对论性无自旋氢原子的解析波函数,推导出了计算径向矩阵元的通项公式.在-6≤s≤3的条件下,给出了径向平均值〈n′l′|rs|n′l′〉的解析表达式.     

关于三维各向同性谐振子径向矩阵元计算的讨论

根据广义Laguerre多项式的数学性质，导出了较为简单的三维各向同性谐振子径向矩阵元的普遍公式,并在这基础上计算了一些重要特殊情形的径向矩阵元: 矢径r整数次幂的平均值，电偶极跃迁矩阵元和电四极跃迁矩阵元. 关键词： 三维各向同性谐振子 径向矩阵元 广义Laguerre多项式 偶极跃迁 四极跃迁     

环形非球谐振子势Klein-Gordon方程的束缚态

用分离变量方法讨论了在环形非球谐振子标量势和矢量势相等条件下的Klein-Gordon方程的束缚态解.给出了用广义连带勒让得多项式表示的归一化角向波函数和用合流超几何函数表示的归一化径向波函数，获得了精确的束缚态能谱方程. 关键词： 环形非球谐振子势 Klein-Gordon方程 束缚态     

Numerical test of approximate theories of the superconducting transition temperature

Various equations for t_c obtained from approximations to the Eliashberg theory are numerically solved and T_cvs λ curves are drawn. Specifically, the weak coupling Kirzhnits, Maksimov and Khomskii (KMK) equation, Eliashberg equation and BCS equation with Bardeen Pines interaction are considered with the α²F function of Nb. The KMK equation gives quite a high value or T_c and the BCS equation overestimates T_c by an even larger factor when compared with the results of the Eliashberg equation.     

Renormalization of the Lorentz-Abraham-Dirac equation for radiation reaction force in classical electrodynamics

Dirac’s analysis of radiation reaction force in classical electrodynamics suggested that a 4-momentum not collinear with 4-velocity could be introduced for a radiating electron. This would be equivalent to renormalization of the electron mass as an operator relating these 4-vectors. Dirac also pointed to an arbitrary choice made in deriving the Lorentz-Abraham-Dirac (LAD) equation. It was shown that renormalization substantially modifies the LAD equation under the additional requirement that the standard relativistic relation ℰ² = p ² c ² + m ² c ⁴ holds for the renormalized energy and momentum. The renormalized LAD equation is more rigorous than the LAD equation, because the drawbacks of the latter are eliminated, and is simpler than a well-known approximation of the LAD equation. The renormalized LAD equation appears to be better suited for numerical simulations of processes in ultrahigh-intensity laser-pulse fields.     

Field theory onR×S 3 topology. I: The Klein-Gordon and Schrödinger equations

A Klein-Gordon-type equation onR×S ³ topology is derived, and its nonrelativistic Schrödinger equation is given. The equation is obtained with a Laplacian defined onS ³ topology instead of the ordinary Laplacian. A discussion of the solutions and the physical interpretation of the equation are subsequently given, and the most general solution to the equation is presented.     

一类相对论性非球谐振子系统的束缚态

给出了具有形式为12r²+A2r²的非球谐振子型标量势和矢量势 的相对论系 统在两种势相等的条件下三维Klein-Gordon方程，二维和三维Dirac方程的s波束缚态解. 关键词： 三维非球谐振子势 Klein-Gordon方程 Dirac方程 束缚态     

一类非线性演化方程新的显式行波解

借助Mathematica软件,采用三角函数法和吴文俊消元法,获得了一类非线性演化方程u_tt+au_xx+bu+cu³=0的三组行波解,其中包括新的行波解、扭状孤波解和钟状孤波解.从而作为该方程的特例,如Duffing方,Klein-Gordon方程、Landau-Ginburg-Higgs方程和⁴方程等也都获得了相应的若干行波解.这种方法也适用于其他非线性方程. 关键词：     

Description of isovector giant dipole resonances in relativistic Vlasov equation at small amplitude limit

A more general relativistic Vlasov equation has been derived in the framework of relativistic quantum hadron dynamical theory. In the small amplitude limit we use this Vlasov equation to study the isovector giant dipole resonances built on groundstate in spherical nuclei¹⁶O,⁴⁰Ca,⁹⁰Zn and²⁰⁸Pb. The results show that the spin-orbit coupling and the non-linear terms of scalar meson can influence the resonance energies to a certain extent comparing with those obtained from the non-relativistic Vlasov equation approach and are in good agreement with the experimental ones, especially for the case which vacuum fluctuation is included.     

Ion volumes and an equation of state for plasma

A plasma equation of state in a gas domain is derived from Saha model accounting for ion cores. Calculations for Cu are performed using the stiff ion core model for densities of up to 10⁶ g/cm³. A compressible ion core model is also developed. The Tomas–Fermi model is applied to condensed plasma. Both models are unified into a thermodynamically consistent equation of state.     

非谐振子势的精确解和双波函数描述

求解了非谐振子势V(x)=x²/2+g/2x²的本征方程，给出了精确的能谱方程和归一化波函数.应用双波函数理论，得到了在非谐振子势场中单粒子运动状态的力学量的时间演化方程. 关键词：     

Soliton-like solutions of some nonlinear theories and transformations among them

The observation that the soliton-like solutions of a given second-order nonlinear differential equation define the separatrix of the equivalent autonomous system is used to obtain the one-soliton solutions for theφ ⁴ theories (the usual and the one with the wrong sign of the mass term), theφ ⁶, theφ ⁸, the sine-Gordon theories and the KdV equation. Transformations are given which transform the sine-Gordon equation into an equation belonging to theφ ²ⁿ class of theories. A procedure is evolved for obtaining the two-soliton solutions for the sine-Gordon theory without the use of Backlund transformations; it is suggested that this procedure may be useful for investigating the existence of similar solutions for theories of the polynomial type.     

A discussion of the relativistic equal-time equation

Ruan Tu-nan et al. [1] have proposed an equal-time equation for composite particles which is derived from Bethe-Salpeter (B-S) equation. Its advantage is that the kernel of this equation is a completely definite single rearrangement of the B-S irreducible kernel without any artificial assumptions. In this paper we shall give a further discussion of the properties of this equation. We discuss the behaviour of this equation as the mass of one of the two particles approaches the limitM ₂→∞ in the ladder approximation of single photon exchange. We show that up to orderO(α⁴) this equation is consistent with the Dirac equation. If the crossed two photon exchange diagrams are taken into account the difference between them is of orderO(α⁶).