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The effective polarization and magnetization fields in terms of charge-current densities

机译:根据电荷电流密度的有效极化场和磁化场

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In the context of electrodynamics of continuous media, the electromagnetic response of a generic medium is usually described in terms of the polarization and magnetization fields P(r, t) and M(r, t), the physical content of which is connected to the multipole expansion of the response of the medium. In this paper, the formal definition of effective polarization and magnetization fields is discussed, these fields being dealt with as potentials of a gauge transformation that is shown to be a particular case of the Serdyukov-Fedorov duality transformation. On the basis of the basic connections of the charge-current densities to the polarization-magnetization potentials, a specific and novel form for P(r, t) and M(r, t) is obtained and the gauge functions whose spatial and temporal derivatives transform such potentials into another equivalent set are determined.
机译:在连续介质的电动力学方面,一般介质的电磁响应通常用极化和磁化场P(r,t)和M(r,t)来描述,它们的物理内容与多极膨胀反应的介质。在本文中,讨论了有效极化场和磁化场的形式定义,这些场被视为规范变换的潜力,这被证明是Serdyukov-Fedorov对偶变换的特殊情况。基于电荷电流密度与极化磁化电势的基本联系,获得了P(r,t)和M(r,t)的特定新颖形式,以及其时空导数的轨距函数确定将这些电势转换为另一个等效集。

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