电偶极振子电场的图示(续)

6　电偶极振子的Ｅｃ 线图图 2中Ｆ(ｒ,π/2 ,ｔ)图线的零点 ,极值点、拐点等反映了什么 ?为说明这些问题我们需先作电偶极振子的Ｅｃ 线图 .在 φ =φ0 (定值 )的平面内 ,Ｅｃ 线满足的微分方程是ｄｒＥｃｒ=ｒｄθＥｃθ将式 ( 4)代入上式 ,消去相同因子 ,得ｄｒ2ｃｏｓθ=ｒｄθｓｉｎθ即 ｄｒｒ =2 ｃｏｓθｄθｓｉｎθ =ｄ(ｓｉｎ2 θ)ｓｉｎ2 θ解上式得 1ｒｓｉｎ2 θ=恒量 ( 1 4′)或　Ｇ(ｒ,θ) =1ｋｒｓｉｎ2 θ=Ｋ(恒量 )　　 ( 1 4 )式 ( 1 4 )中ｋ仍为 ｗｃ,值得注意Ｅｃ 线形状不随时间变化 .用类似于求Ｅ线的作图法画出Ｅ…     

浅谈偶极振子辐射的图示

指出了目前物理教学中在偶极振子辐射的图示方面存在的一些问题,并就这些问题进行了分析、探讨。     

推算偶极振子电磁场的简单方法

偶极振子电磁场的分布和变化规律可以由麦克斯韦方程组严格计算出来，但由于计算繁杂和数学知识的限制，电磁学书中只进行定性讨论或直接给出结果再进行分析，学生不易接受．本文提出的图象、量纲分析法使偶极振子电磁场的求解大为简化，且物理概念清晰，在教学实践中效果较好．     

FeXXI离子电偶级、磁偶极及电四极跃迁振子强度的计算

讨论了使用MCHF方法优化径向波函数以获取大量原子参数的方法，由得到的波函数计算了FeXXI离子的相对论与非相对论能级，将计算能级与已有的实验结果进行了比较，对电偶极，磁偶极以及电四极的振子强度进行了非相对论与相对论修正的计算，对非相对论计算的振子强度，长度与速度两种表示符合较好。     

关于ψ(3770)的电偶极跃迁

本文采用一种以QCD为基础的势模型,计算了cc态的各种E1跃迁宽度.结果表明相对论修正效应相当重要.所得ψ(2s)→γχ_cJ和χ_cJ→γψ(1S)(J=0,1,2)的跃迁宽度与实验符合,但ψ(3770)→γχ_cJ跃迁宽度要比MarkⅢ实验组的新近结果小2倍左右.改善理论结果的一个可能性是考虑2³S₁—1³D1混合的效应.     

S-D混合与ψ(3770)的电偶极跃迁

本文在粲偶素势模型的框架内,讨论了ψ(3770)与ψ(3686)之间的2³S₁-1³D₁混合对ψ(3770)与ψ(3686)电偶极跃迁的影响.结论是混合角θ=30°应予排除,而θ=－10°虽然可以对ψ(3770)→χ₀γ和ψ(3686)→χ₀γ给出改善的结果,但仍不能解决ψ(3770)→χ₁γ与实验的矛盾.     

偏振光激发的Sr原子电偶极辐射

原子与激光场相互作用产生的自发辐射可以用经典电偶极辐射理论很好的描述.通过改变与Sr原子束相互作用激光的偏振方向,分析探测Sr原子束荧光强度的变化,测定了在远场区的电偶极辐射特性.Sr原子电偶极子在远场区辐射能量的空间方向分布满足sin2θ关系,利用这一规律可以有效地探测到最强的荧光光谱.     

高温转动核的电偶极巨共振研究

简要叙述了高温转动核电偶极巨共振实验研究的历史和现状，并着重介绍了现存的一些问题及新的探索． The history and current status of the experimental study of giant dipole resonance in hot rotating nuclei has been reviewed.Some open problems and new development are stressed.     

量子力学偶极求和规则和ψ(3770)的电偶极跃迁

本文对量子力学偶极求和规则进行了一些普遍的讨论.利用这些求和规则估算了ψ(3770)的电偶极跃迁宽度的上限和下限.结果表明.Mark Ⅲ组给出的实验值明显偏大.     

Quantum holonomies for an electric dipole moment

In this Letter, we obtain the quantum holonomies for a neutral particle with a permanent electric dipole moment based on the analogue effects of the He-McKellar-Wilkens effect and the Scalar Aharonov-Bohm effect and show a new proposal for implementing one-qubit quantum gates.     

Transmission of electric dipole radiation through an interface

We consider the transmission of electric dipole radiation through an interface between two dielectrics, for the case of a vertical dipole. Energy flows along the field lines of the Poynting vector, and in the optical near field these field lines are curves (as opposed to optical rays). When the radiation passes through the interface into a thicker medium, the field lines bend to the normal (as rays do), but the transmission angle is not related to the angle of incidence. The redirection of the radiation at the interface is determined by the angle dependence of the transmission coefficient. This near-field redistribution is responsible for the far-field angular power pattern. When the transmission medium is thinner than the embedding medium of the dipole, some energy flows back and forth through the interface in an oscillating fashion. In each area where field lines dip below the interface, an optical vortex appears just above the interface. The centers of these vortices are concentric singular circles around the dipole axis.     

The electric dipole moment of the muon

The forthcoming experiment [1] on the anomalous magnetic moment of the muon will be able to search also for an electric dipole momentd _μ of the muon with increased sensitivity. A brief survey is given on what various models of CP violation predict ford _μ.     

The electric dipole moment of methyl fluoride

The Stark effect of CH₃F is extensively used as a calibration standard in laser Stark spectroscopy. The accepted value for the dipole moment of the ground vibrational state of CH₃F is less accurate than the precision of laser Stark measurements, and questions have also been raised about the literature value. New molecular beam spectroscopy measurements have been made of the ratio of the Stark effect in the J = 1, K = 1 and J = 2, K = 2 CH₃F states to that of the 01¹0 vibrational state of OCS. The results were $\text{μ}{}_{1.1}\text{(}\text{CH}{}_3\text{F}\text{)}\text{μ}{}_{010}\text{(}\text{OCS}\text{)}\text{= 2.638905(23)}$ and $\text{μ}{}_{2.2}\text{(}\text{CH}{}_3\text{F}\text{)}\text{μ}{}_{010}\text{(}\text{OCS}\text{)}\text{= 2.63894(10)}$. This produces a dipole moment of 1.85840 D with precision relative to OCS of 10 ppm and absolute accuracy of 43 ppm.     

Phase diagram of water under an applied electric field

Simulations are used to investigate for the first time the anisotropy of the dielectric response and the effects of an applied electric field E(ex) on the phase diagram of water. In the presence of electric fields ice II disappears from the phase diagram. When E(ex) is applied in the direction perpendicular to the ac crystallographic plane the melting temperatures of ices III and V increase whereas that of ice Ih is hardly affected. Ice III also disappears as a stable phase when E(ex) is applied in the direction perpendicular to the ab plane. E(ex) increases by a small amount the critical temperature and reduces slightly the temperature of the maximum density of liquid water. The presence E(ex) modifies all phase transitions of water but its effect on solid-solid and solid-fluid transitions seems to be more important and different depending on the direction of E(ex).