The divergence of the Weyl tensor 
First, the Weyl tensor is given by
  $$W_{ijkl}=R_{ijkl}-\frac{1}{n-2}(g_{ik}A_{jl}-g_{il}A_{jk}-g_{jk}A_{il}+g_{jl}A_{ik})$$
  where, $A_{ij}$ is the Schouten tensor, given by
  $$A_{ij}=R_{ij}-\frac{R}{2(n-1)}g_{ij}$$ And the Cotton tensor is
  given by $$C_{ijk}=\nabla_{i}A_{jk}-\nabla_{j}A_{ik}$$ I've to show
  that the divergence of the Weyl tensor and the Cotton tensor satisfy:
  $$C_{ijk}=-\frac{n-2}{n-3}\nabla_{l}W_{ijkl}\qquad(*)$$

I know that the divergence of the Weyl tensor is $g^{ls}\nabla_sW_{ijkl}$ and, by the once contracted second Bianchi identity is $g^{ls}\nabla_sR_{ijkl}=-\nabla_iR_{jk}+\nabla_jR_{ik}$.
Someone can help me to show the identity $(*)$?
 A: First note that
$$\nabla^l A_{jl}=\nabla^l R_{jl}-\nabla^l \frac{R}{2(n-1)}g_{jl}=\nabla^l R_{jl}- \frac{1}{2(n-1)}\nabla_j R=\frac{1}{2}\nabla_j R- \frac{1}{2(n-1)}\nabla_j R=\frac{n-2}{2(n-1)}\nabla_j R \qquad(1)$$
the last equality is obtained by twice contracted second Bianchi identity ( that is $2\nabla^jR_{jk}=\nabla_k R$)
Now we calculate the divergence of the Weyl tensor:
$$g^{ls}\nabla _sW_{ijkl}=g^{ls}\nabla_s R_{ijkl}-\frac{1}{n-2}(g_{ik}g^{ls}\nabla_s A_{jl}-g_{il}g^{ls}\nabla_s A_{jk}-g_{jk}g^{ls}\nabla_s A_{il}+g_{jl}g^{ls}\nabla_s A_{ik})$$
$$=\nabla_iR_{jk}-\nabla_jR_{ik}-\frac{1}{n-2}(g_{ik}\nabla^l A_{jl}-g_{il}\nabla^l A_{jk}-g_{jk}\nabla^l A_{il}+g_{jl}\nabla^l A_{ik})$$
$$=\nabla_iR_{jk}-\nabla_jR_{ik}-\frac{1}{n-2}(g_{ik}\nabla^l A_{jl}-\nabla_i A_{jk}-g_{jk}\nabla^l A_{il}+\nabla_j A_{ik})$$
We know $C_{ijk}=\nabla_{i}A_{jk}-\nabla_{j}A_{ik}$, then
$$=\nabla_iR_{jk}-\nabla_jR_{ik}-\frac{1}{n-2}(g_{ik}\nabla^l A_{jl}-g_{jk}\nabla^l A_{il}-C_{ijk})$$
Now by considering (1):
$$=\nabla_iR_{jk}-\nabla_jR_{ik}-\frac{1}{n-2}(g_{ik}\frac{n-2}{2(n-1)}\nabla_j R-g_{jk}\frac{n-2}{2(n-1)}\nabla_i R-C_{ijk})$$
$$=\nabla_iR_{jk}-\nabla_jR_{ik}-\frac{1}{2(n-1)}g_{ik}\nabla_j R+\frac{1}{2(n-1)}g_{jk}\nabla_i R+\frac{1}{n-2}C_{ijk}$$
$$=\nabla_i(R_{jk}+\frac{R}{2(n-1)}g_{jk})-\nabla_j(R_{ik}+\frac{R}{2(n-1)}g_{ik})+\frac{1}{n-2}C_{ijk}$$
By using $\frac{R}{2(n-1)}g_{ij}=R_{ij}-A_{ij}$:
$$=\nabla_i(2R_{jk}-A_{jk})-\nabla_j(2R_{ik}-A_{ik})+\frac{1}{n-2}C_{ijk}$$
$$=2\nabla_i R_{jk}-2\nabla_j R_{ik}-\nabla_iA_{ik}+\nabla_jA_{ik}+\frac{1}{n-2}C_{ijk}=-C_{ijk}+\frac{1}{n-2}C_{ijk}=-\frac{n-3}{n-2}C_{ijk}$$
Note that $2\nabla_i R_{jk}-2\nabla_j R_{ik}=0$. So we obtain

$$C_{ijk}=-\frac{n-2}{n-3}g^{ls}\nabla _sW_{ijkl}=-\frac{n-2}{n-3} \nabla^l W_{ijkl}$$

