Abstract
Close to the position \(\mathbf {y}(t)\) of a charged particle, the electromagnetic field it creates diverges as \(F^{\mu \nu }\sim 1/ r^2\), where \(r=|\mathbf {x}-\mathbf {y}(t)|\) is the distance from the particle. Correspondingly, the electromagnetic energy-momentum tensor
diverges as
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Notes
- 1.
The prescribed test function space would be \(\mathcal{S}(\mathbb {R}^4)\). However, since in the static case the dependence on the time variable t is trivial, it is not restrictive to consider the spatial test function space \(\mathcal{S}(\mathbb {R}^3)\).
- 2.
As the characteristic function \(\chi _V(\mathbf {x})\) is not continuous in \(\mathbb {R}^3\), it is actually not an element of \(\mathcal{S}(\mathbb {R}^3)\). Consequently, a priori the quantities \(\mathbb {T}^{00}_\mathrm{em}(\chi _V)\) are ill-defined. This problem can be remedied in a rigorous way, by “approximating” \(\chi _V(\mathbf {x})\) with a sequence of functions \(\chi _V^n(\mathbf {x})\in \mathcal{S}(\mathbb {R}^3)\) such that almost everywhere \(\lim _{n\rightarrow \infty }\chi _V^n(\mathbf {x}) = \chi _V(\mathbf {x})\), and by defining then \(\mathbb {T}^{00}_\mathrm{em}(\chi _V)\) as the limit \(\lim _{n\rightarrow \infty } \mathbb {T}^{00}_\mathrm{em}(\chi _V^n)\).
References
K. Lechner, P.A. Marchetti, Variational principle and energy-momentum tensor for relativistic electrodynamics of point charges. Ann. Phys. 322, 1162 (2007)
K. Lechner, Radiation reaction and four-momentum conservation for point-like dyons. J. Phys. A 39, 11647 (2006)
E.G.P. Rowe, Structure of the energy tensor in the classical electrodynamics of point particles. Phys. Rev. D 18, 3639 (1978)
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Lechner, K. (2018). Renormalization of the Electromagnetic Energy-Momentum Tensor. In: Classical Electrodynamics. UNITEXT for Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-91809-9_16
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DOI: https://doi.org/10.1007/978-3-319-91809-9_16
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