玻恩-因菲尔德电动力学中的光子-光子散射

H. Kadlecová
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摘要

本文在玻恩-因菲尔德电动力学中研究了真空中两个反向传播电磁波的相互作用。首先,我们研究了线极化光束的玻恩情况,E·B = 0,即G2 = 0(交叉场结构),这与玻恩-因菲尔德和玻恩的电动力学相同;然后,我们研究了非线性极化,G2≠0的光束的一般玻恩-因菲尔德情况。在这两种情况下,我们用自相似解证明了非线性场方程解耦,并研究了激波的形成。我们证明了唯一的非线性解是例外的行波解,它以恒定的速度传播并且不会变成冲击。在玻恩的情况下,我们自然地得到了反传播(实光子-光子散射)和共传播(非相互作用)光束方向的例外波解,我们研究了它们的传播方向。在Born - infeld情况下,我们还选择了相速度恒定的解来匹配Born情况下背景场相速度的极限。我们得到了两种异常波解,然后我们数值分析了哪个相速度对应于反传播或共传播光束,然后我们确定了异常波的传播方向。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Photon-photon scattering in Born-Infeld electrodynamics
We study the interaction of two counter–propagating electromagnetic waves in vacuum in the Born–Infeld electrodynamics. First we investigate the Born case for linearly polarized beams, E · B = 0, i. e. G2 = 0 (crossed field configuration), which is identical for Born–Infeld and Born electrodynamics; subsequently we study the general Born–Infeld case for beams which are nonlinearly polarized, G2 ≠ 0. In both cases, we show that the nonlinear field equations decouple using self-similar solutions and investigate the shock wave formation. We show that the only nonlinear solutions are exceptional travelling wave solutions which propagate with constant speed and which do not turn into shocks. In the Born case, we naturally obtain exceptional wave solutions for counter–propagating (real photon– photon scattering) and for a co–propagating (non-interacting) beam orientation we investigate their direction of propagation. In the Born–Infeld case, we have additionally chosen the solutions which have constant phase velocities to match the limits of phase velocities of the background field in the Born case. We obtain two types of exceptional wave solutions, then we numerically analyze which phase velocities correspond to the counter– or co–propagating beams and subsequently we determine the direction of propagation of the exceptional waves.
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