2003
DOI: 10.1088/0264-9381/20/13/313
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New electromagnetic conservation laws

Abstract: The Chevreton superenergy tensor was introduced in 1964 as a counterpart, for electromagnetic fields, of the well-known Bel-Robinson tensor of the gravitational field. We here prove the unnoticed facts that, in the absence of electromagnetic currents, Chevreton's tensor (i) is completely symmetric, and (ii) has a trace-free divergence if Einstein-Maxwell equations hold. It follows that the trace of the Chevreton tensor is a rank-2, symmetric, trace-free, conserved tensor, which is different from the energy-mom… Show more

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Cited by 27 publications
(53 citation statements)
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“…However, the tensor versions are of varying degrees of difficulty: the familiar Bel-Robinson identity in Theorem 2a requires considerable preliminary work to establish lemmas for the Weyl tensor, and Theorem 2d requires Theorem 2a together with a number of other lemmas, one involving a 'mixed' identity. The tensor derivation of the new conservation law for electromagnetism [5] given in Section 7 also requires 'mixed' ddis. These tensor derivations are very complicated, and one wonders how long it would have taken to even conjecture the results in Theorems 2d and 6 without the parallel spinor (or null vector) results; but it seems that there is no easier signature-free way in tensors, and we should train ourselves to recognise such structures in tensors.…”
Section: Discussionmentioning
confidence: 99%
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“…However, the tensor versions are of varying degrees of difficulty: the familiar Bel-Robinson identity in Theorem 2a requires considerable preliminary work to establish lemmas for the Weyl tensor, and Theorem 2d requires Theorem 2a together with a number of other lemmas, one involving a 'mixed' identity. The tensor derivation of the new conservation law for electromagnetism [5] given in Section 7 also requires 'mixed' ddis. These tensor derivations are very complicated, and one wonders how long it would have taken to even conjecture the results in Theorems 2d and 6 without the parallel spinor (or null vector) results; but it seems that there is no easier signature-free way in tensors, and we should train ourselves to recognise such structures in tensors.…”
Section: Discussionmentioning
confidence: 99%
“…Recently Bergqvist, Eriksson and Senovilla [5] have used the spinor equivalent of the Chevreton tensor and given two interesting properties in curved space for source-free Einstein-Maxwell fields:…”
Section: Tensor Derivation Of New Electromagnetic Conservation Lawmentioning
confidence: 99%
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“…Bergqvist, Eriksson and Senovilla (BES) [2] have recently found that the trace of the Chevreton tensor [3], [4],…”
mentioning
confidence: 99%