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The Geometry of Regular Shear-Free Null Geodesic Congruences, CR functions and their Application to the Flat-Space Maxwell Equations

机译:常规无剪切空间测地同余的几何,CR   函数及其在平 - 空麦克斯韦方程组中的应用

摘要

We describe here what appears to be a new structure that is hidden in allasymptotically vanishing Maxwell fields possessing a non-vanishing totalcharge. Though we are dealing with real Maxwell fields on real Minkowski spacenevertheless, directly from the asymptotic field one can extract a complexanalytic world-line defined in complex Minkowski space that gives a unifiedLorentz invariant meaning to both the electric and magnetic dipole moments. Insome sense the world-line defines a `complex center of charge' around whichboth electric and magnetic dipole moments vanish. The question of how and where does this complex world-line arise is one ofthe two main subjects of this work. The other subject concerns what is known inthe mathematical literature as a CR structure. In GR, CR structures naturallyappear in the physical context of shear-free (or asymptotically shear-free)null geodesic congruences in space-time. For us, the CR structure is associatedwith the embedding of Penrose's real three-dimensional null infinity, I^+, as asurface in a two complex dimensional space, C^2. It is this embedding, via acomplex function, (a CR function), that is our other area of interest.Specifically we are interested in the `decomposition' of the CR function intoits real and imaginary parts and the physical information contained in thisdecomposition.
机译:我们在这里描述似乎是一种新结构,它隐藏在拥有不消失的总电荷的所有渐近消失的麦克斯韦场中。尽管我们正在处理实际Minkowski空间上的实际Maxwell场,但可以直接从渐近场中提取在复杂Minkowski空间中定义的复杂分析世界线,从而为电偶极矩和磁偶极矩提供统一的洛仑兹不变性。从某种意义上说,世界线定义了一个“复杂的电荷中心”,电偶极矩和磁偶极矩都消失了。这个复杂的世界线如何以及在何处出现的问题是这项工作的两个主要主题之一。另一个主题涉及数学文献中称为CR结构的问题。在GR中,CR结构自然出现在时空无切变(或渐近无切变)零大地测全等的物理环境中。对我们来说,CR结构与Penrose的真实三维零位无穷大I ^ +的嵌入在二维复维空间C ^ 2中相关联。正是通过复杂函数(CR函数)的这种嵌入才成为我们关注的另一个领域。特别是,我们对CR函数“分解”为实部和虚部以及此分解中包含的物理信息感兴趣。

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