So, i'm going over the Thorne's derivation of the quadrupolar radiation term, and they write the core term as:
$$ \frac{3 r_i r_j - 2 r^2 \delta_{ij}}{4 r^5} $$
But if i try to obtain this term by Covariant deriving the dipole term;
$$ \nabla_{ij}{ \frac{1}{r}} = - \nabla_{j}{ \frac{r_i}{2 r^3}} $$
i am left with:
$$ \frac{3 r_i r_j - 2 r^2 \delta_{ij}}{4 r^5} - \frac{\Gamma^i_{kj}r_k}{2r^3} $$
Where the last term seems to be dismissed in the text with no good reason. Is there a reason why this term is being ignored?