My question is simple. Let $X^{\mu\nu}$ be a rank-2 tensor, and $\nabla_\mu$ be the metric compatible, torsion-free, covariant derivative. Does the identity $(\nabla_\mu \nabla_\nu - \nabla_\nu \nabla_\mu) X^{\mu\nu}=0$ holds ? My proof goes like this
- Write the definition of the Riemann $(\nabla_\mu \nabla_\nu - \nabla_\nu \nabla_\mu) X^{\mu\nu} = -\frac{1}{2}(R_{\mu\nu\lambda}^{\phantom{\mu\nu\lambda}\mu}X^{\lambda\nu}+R_{\mu\nu\lambda}^{\phantom{\mu\nu\lambda}\nu}X^{\mu\lambda})$.
- Rename the indices $\mu\leftrightarrow\nu$ in the first term on the right, and use the antysymmetry $R_{\mu\nu\lambda}^{\phantom{\mu\nu\lambda}\nu}=-R_{\mu\nu\lambda}^{\phantom{\mu\nu\lambda}\mu}$ of the Riemann tensor, to get $(\nabla_\mu \nabla_\nu - \nabla_\nu \nabla_\mu) X^{\mu\nu} = -\frac{1}{2}(-R_{\mu\nu\lambda}^{\phantom{\mu\nu\lambda}\nu}X^{\lambda\mu}+R_{\mu\nu\lambda}^{\phantom{\mu\nu\lambda}\nu}X^{\mu\lambda})$.
- Introduce the symmetric Ricci tensor $R_{\mu\lambda}:=R_{\mu\nu\lambda}^{\phantom{\mu\nu\lambda}\nu}$, to get finally $(\nabla_\mu \nabla_\nu - \nabla_\nu \nabla_\mu)X^{\mu\nu} = \frac{1}{2}R_{\mu\lambda}(X^{\lambda\mu}-X^{\mu\lambda})$
- That last term is the contraction of $R_{\mu\lambda}$ (symmetric) and $X^{\lambda\mu}-X^{\mu\lambda}$ (anti-symmetric), therefore vanishes.
This seems to be true for any $X^{\mu\nu}$, but the result seems quite strong, and I've never seen it anywhere.
Anybody can confirm and/or see a mistake in my reasoning ?
Thanks
This is correct. Here's another way to see it: Decompose $X^{\mu\nu}=A^{\mu\nu}+B^{\mu\nu}$ into its symmetric and skew symmetric parts $A^{\mu\nu}$ and $B^{\mu\nu}$, respectively. For your 4th reason, $(\nabla_\mu\nabla_\nu-\nabla_\nu\nabla_\mu)A^{\mu\nu}=0$. The fact $(\nabla_\mu\nabla_\nu-\nabla_\nu\nabla_\mu)B^{\mu\nu}=0$ follows from the fact $\delta^2=0$, where $\delta$ is the divergence on differential forms; this is the dual of the identity $d^2=0$. More precisely, $$ (\nabla_\mu\nabla_\nu-\nabla_\nu\nabla_\mu)B^{\mu\nu}=-2\nabla^\nu\nabla^\mu B_{\mu\nu} = -2\delta^2B = 0 . $$ (I raised and lowered indices just to emphasize that $\delta$ is the divergence.)