旋转带电体和电磁场的角动量守恒定律及能量守恒定律

对均匀带电薄球壳匀加带旋转问题,由电磁场的角动量定恒守律和能量守恒定律两种方法分别得出了外力矩力其功率的正确正确结果。     

电容器和螺绕环转动时电磁场的角动量

分别计算了理想的圆柱形电容器、 圆形平行板电容器和螺绕环这三者绕各自中心对称轴做定轴转动 时电磁场对转轴的角动量.计算结果或许没有什么实用价值, 但应该具有一定的理论认识价值, 即该计算结果从一 个侧面体现了电磁场这种物质形态的一点特殊性     

电磁场角动量守恒定律的又一例

处于外磁场中圆柱形带电体，当外磁场变化时，带电体将旋转，本文分别用电磁体系的能量守恒和角动量守恒对其进行讨论，说明它们的一致。     

电磁场角动量守恒及其应用

由带电体与电磁场相互作用时角动量守恒推导出电磁场角动量及角动量流的具体表达式,讨论了电磁角动量对于深入理解电磁场基本属性的作用以及它在微观物理学研究中的应用。     

两个佯谬—关于静场量物理真实性的讨论

通过对两个事例的严格讨论，明确了静场动理和角动量的物理真实性。     

费曼圆盘佯谬及角动量守恒

简述电磁场中角动量守恒定律和费曼圆盘佯谬，对描述费曼圆盘的模型进行了讨论，最后对静场远区的角动量作了定量计算。     

费曼佯谬与电磁场角动量守恒

带电体在转动过程中，机械和电磁场联合系统角动量守恒，本文首先介绍费曼佯谬，然后从理论上提出电磁场角动量的概念，导出电磁场角动量守恒定律，并用带电体与电磁场联合系统角动量守恒的原理揭示了费曼转盘转动的机理。     

电磁学与电动力学中的磁单极-I

本文及后继三篇文章在电磁学和电动力学框架内分别介绍磁单极的若干奇特性质.针对由一个磁单极和一个点电荷构成的体系,首先证明这个体系的电磁场角动量具有极简洁的表达式并讨论可能的电荷量子化,然后显式地演示体系角动量的转化与守恒.     

电磁场边值关系的推广应用

本文把磁场边值关系推广应用于介质分界面上或存在自由电荷面分布，自由电流线分 布的曲面上的任意曲面，使解某些具有特殊结构的电磁场边值问题，物理图象更清晰，意义更直观明了。     

刚体角动量的定义和定义状态量的原则

从圆周运动质点的角动量出发,分析了定轴转动刚体角动量定义的合理性和惟一性;阐述定义状态量的原则;给出一种推导转动定律的方法;阐明把定轴转动刚体作为特殊质点系的逻辑一致性．     

Contribution of Electromagnetic Field to Atomic Spin

We examine the contribution of electromagnetic field to the atomic spin, by adopting two different, both gauge invariant definitions of the electromagnetic angular momentum: \vec{J}_I ≡ ∫d³ x ε₀ \vec{r} X (\vec{E} X \vec{B}) and \vec{J}_II ≡ ∫d³ x ( ε₀ \vec{E} X \vec{A}^\bot + ε₀ E_i \vec{r} X \vec{\nabla }A^{\bot}_i ). Notably, at the classical level, \vec{J}_II gives an exactly null result while \vec{J}_I gives a finite value. This suggests that \vec{J}_II leads to a simpler and more reasonable picture of the atomic spin, therefore qualifies as a more appropriate definition of the electromagnetic angular momentum. Our observation gives important hint on the delicate issue of gluon contribution to the nucleon spin.     

Orbital angular momentum of channeling radiation from relativistic electrons in thin Si crystal

We propose to use channeling radiation (CR) from relativistic electrons as a source of high energy twisted photons in the MeV range. We calculate numerically the orbital angular momentum (OAM) of radiation produced by electrons with the energies $155÷2500$ MeV for the axial and planar channeling in the thin Si crystal. We obtain that the average OAM of CR in this case is approximately $1÷6?$ per photon with the photon energies about $1÷2$ MeV.     

Effects of magnetic field on the evolution of the wave function of a charged particle with an angular momentum

We have calculated the effect of a magnetic field on the evolution of angular momentum eigenfunctions of a charged particle. An additional harmonic potential is supplemented to trap the wave packet. We find the probability density of the wave function is oscillating in the radial direction with a time period determined by the strength of the effective harmonic potential. When the magnetic field is along the z direction, if the initial wave function is an eigenfunction of ${\hat{L}}_{z}$, the probability density of the particle remains axis-symmetric. While for the case of an eigenfunction of ${\hat{L}}_{x}$, it is anisotropic in the x−y plane and rotates with a time period inverse proportional to the strength of the external magnetic field. We also extend the results in a phenomenological way to the case with an external magnetic field that varies harmonically in time.     

20MeV到180MeV／u~（16）O＋~（197）Au系统的BUU计算：线动量与角动量转移依赖碰撞参数与能量研究

用考虑了角动量守恒的ＢＵＵ模型计算了２０ＭｅＶ≤Ｅ／ｕ≤１８０ＭｅＶ能区１６Ｏ＋１９７Ａｕ系统的反应线性动量转移（ＬＭＴ）及余核角动量，着重讨论了反应线性动量转移及余核角动量对反应碰撞参量、入射能Ｅ／ｕ的依赖关系，比较了计算ＬＭＴ与Ｖｉｏｌａ系统性给出的结果间的偏差．计算结果揭示了当Ｅ／ｕ≥９０ＭｅＶ时，余核角动量对Ｅ／ｕ增长出现的饱和现象，主要来源于靶核对弹核捕获能力的持续丢失．     

推导平方反比有心力场中质点轨道的一种方法

根据动量定理和角动量定理，通过直角坐标系和平面极坐标系单位矢量的变换，给出了推导平方反比有心力场中轨道的一种新方法．     

Shared aperture metasurface antenna for electromagnetic vortices generation with different topological charges

Vortex beams carrying orbital angular momentum (OAM) have aroused great interest of both scientific and engineering communities. Encouragingly, generating OAM with different topological charges in a shared aperture is regarded as a potential route to expanding the communication capacity, which yet is an academic challenging task. In this work, a paradigm of designing metasurface-based shared aperture antenna for generating polarization-dependent vortex beams with distinct topological charges is proposed. Anisotropic unit cells that can tailor different resonance phase profiles in two orthogonal orientations are used to assemble a metasurface reflector. As a proof-of-concept, a planar reflector antenna is designed with two Vivaldi sources, which can generate x- and y-polarized vortex beams with topological charges of l=-1 and l=-2, respectively. Both the simulation results and the measurement results are in good agreement, which demonstrates the feasibility of our design. Significantly, this work provides a new route to achieving vortex beams carrying different topological charges in the same frequency band, which may have potential applications in communication systems.