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| | The Ricci Tensor |
 | | The Ricci tensor arises as a trace of the Riemann tensor which, in turn, is obtained by taking the second derivatives of tensor fields and antisymmetrising over the gradient-rank factors added to the tensor fields' ranks in so doing. |
 | | Now, it so happens that the construction, starting with a differential operator and yielding its Ricci tensor, can actually be applied to a broad class of tensor operators, which I describe as Leibniz operators. |
 | | By construction, this tensor is antisymmetric under interchange of its first two components: this slightly reduces the collection of options to be tried. |
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