关于电磁场的量子化

自由电磁场的量子化意味着它的angular momentum的量子化

Quantization of the free electromagnetic field implies quantization of its angular momentum

结果表明，当自由电磁场的规范不变Bohr-Rosenfeld算符应用于解释为算符的电磁场的线动量和角动量的表达式时，在没有电和磁电荷密度的情况下，这些算符满足动量和角动量的正则对易关系.这证实了它们作为算符的有效性，可以用于角动量的量子力学计算。

关于电磁场量子化问题

On the Problem of Electromagnetic-Field Quantization

我们考虑了具有变化介质的腔体中的辐射场算符，其形式为最一般的一维二次哈密顿量的海森堡运动方程的解。这些方程的显式解决方案，并获得应用程序的辐射场量子化，包括随机变化的媒体，进行了简要讨论。

柱面上的广义Weyl量子化与量子相位

Generalized Weyl quantization on the cylinder and quantum phase

本文发展了圆柱相空间$S^1 \times \mathbb{R}^1$的广义Weyl量子化形式。结果表明，与线性谐振子或电磁场的相位有关的量子观测量可以用Hilbert空间$L^2(S^1)$上的自伴算符表示.

Quantization and soliton-like solutions for the $ΦΨ$-model in a optic fiber

In the framework of a mesoscopical model for dielectric media we provide an analytical description for the electromagnetic field confined in a cylindrical cavity containing a finite dielectric sample. This system is apted to simulate the electromagnetic field in a optic fiber, in which two different regions, a vacuum region and a dielectric one, appear. A complete description for the scattering basis is introduced, together with field quantization and the two-point function. Furthermore, we also determine soliton-like solutions in the dielectric, propagating in the sample of nonlinear dielectr…

广义狄拉克括号和庞加莱对称性在场正则量子化程序中的作用2

Generalized Dirac bracket and the role of the Poincaré symmetry in the program of canonical quantization of fields 2

在这篇文章中，正则分析和量子化的方法，在系列的第一部分审查应用到狄拉克场的情况下，存在电磁相互作用。它表明，量子化的电动力学，它开始于一个给定的拉格朗日和散射概率振幅的微扰计算结束，可以进行的方式，不采用庞加莱对称性的空间-时间在任何阶段。此外，因果结构也是不需要的。

Electromagnetic Potential in Pre-Metric Electrodynamics: Causal Structure, Propagators and Quantization

An axiomatic approach to electrodynamics reveals that Maxwell electrodynamics is just one instance of a variety of theories for which the name electrodynamics is justified. They all have in common that their fundamental input are Maxwell's equations $\textrm{d} F = 0$ (or $F = \textrm{d} A$) and $\textrm{d} H = J$ and a constitutive law $H = # F$ which relates the field strength two-form $F$ and the excitation two-form $H$. A local and linear constitutive law defines what is called local and linear pre-metric electrodynamics whose best known application are the effective description of electro…