电动力学中Lorentz破坏信号的新极限

Radiation Reaction in a Lorentz-Violating Electrodynamics

We study radiation reaction in a Lorentz violating electrodynamics [1]. We explore the possible modification whatsoever present in the radiation reaction force experienced by an accelerating charge in the modified Maxwell theory. However it turns out that radiation reaction receives no change due to Lorentz violation whereas electromagnetic mass manifests anisotropy.

The classical Maxwell-Lorentz electrodynamics aspects of the electron inertia problem within the Feynman proper time paradigm

The Maxwell electromagnetic and the Lorentz type force equations are derived in the framework of the R. Feynman proper time paradigm and the related vacuum field theory approach. The electron inertia problem is analyzed within the Lagrangian and Hamiltonian formalisms and the related pressure-energy compensation principle. The modified Abraham- Lorentz damping radiation force is derived, the electromagnetic electron mass origin is argued.

论经典电动力学中洛伦兹规范与库仑规范的不等价性

On non-equivalence of Lorentz and Coulomb gauges within classical electrodynamics

它表明，众所周知的程序证明等价的电场计算使用洛伦兹和库仑规范的表达式是不正确的。这两种规范之间的差异是由于标量位扰动传播速度的差异。作为一个辅助结果，它证明了电场的解决方案不能直接从麦克斯韦方程组，即不引入标量和矢量势。

洛伦兹电动力学、物质/反物质宇宙学和天体粒子物理

Lorentz Electrodynamics, Matter/Antimatter Cosmology and Astroparticle Physics

证明了非对易洛伦兹度规满足所谓的非传播波。长程力作为这些波动的描述。它导致了场值（群速度和德布罗意波的强度）自然地引入麦克斯韦方程组，反物质自然地引入牛顿力学。波动理论的早期预测之一是反粒子（具有负群速度的模式）的存在。它们被普通物质吸引，但由于引力而排斥普通物质和彼此。这两种物质之间的相互作用可能导致宇宙膨胀，并维持宇宙强辐射源的能量库。

No-go theorem for the classical Maxwell-Lorentz electrodynamics in odd-dimensional worlds

If the conventional Maxwell--Lorentz formulation of classical electrodynamics is adopted in a flat spacetime of arbitrary odd dimension, then the retarded vector potential $A^μ$ generated by a point charge turns out to be pure gauge, $A^μ=\partial^μχ$. By Gauss' law, the charge shows up as zero. The classical electromagnetic coupling is thus missing from odd-dimensional worlds. If the action is augmented by the addition of the Chern--Simons term, then the classical interaction picture in the three-dimensional world becomes nontrivial.

经典电动力学基础的温和介绍：激励（D，H）和场强（E，B）的含义

A gentle introduction to the foundations of classical electrodynamics: The meaning of the excitations (D,H) and the field strengths (E, B)

概述了电磁理论的公理结构。我们将把经典电动力学建立在（1）电荷守恒、（2）洛伦兹力、（3）磁通量守恒和（4）麦克斯韦-洛仑兹时空关系的基础上。这就产生了麦克斯韦方程组。除其他外，还将得出电场和磁场的解释和尺寸的结果。