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Bel–Robinson tensor : ウィキペディア英語版 | Bel–Robinson tensor In general relativity and differential geometry, the Bel–Robinson tensor is a tensor defined in the abstract index notation by: : where is the Weyl tensor. It was introduced by Lluís Bel in 1959. The Bel–Robinson tensor is constructed from the Weyl tensor in a manner analogous to the way the electromagnetic stress–energy tensor is built from the electromagnetic tensor. Like the electromagnetic stress–energy tensor, the Bel–Robinson tensor is totally symmetric and traceless: : : ==References== 〔
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