The covariant derivative of a contravariant tensor (also called the "semicolon derivative"
since its symbol is a semicolon) is given by
|
(1)
| |||
|
(2)
|
(Weinberg 1972, p. 103), where is a Christoffel
symbol of the second kind, Einstein summation
is used in the last term, and
is a comma derivative.
The divergence
is the tensor
contraction of this covariant derivative, a scalar
rather than the full
tensor (Carroll 1997, p. 61).
The covariant derivative of a covariant tensor is
|
(3)
|
(Weinberg 1972, p. 104).
Schmutzer (1968, p. 72) uses the older notation or
.