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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:
:T_=C_C_ _ \epsilon__ C_ C__=C_C_ _ g_" TITLE="b}">C_ C^^
where C_ 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:
:T_=T_
:T^ T_ = 0
==References==



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