In my lectures, we considered the conserved stress energy tensor $T^{\mu \nu}$ and noted that we could always add a conserved tensor to it such that $T^{\mu \nu}$ is symmetric.
As a consequence, a tensor of higher rank, $M^{\lambda \mu \nu}= x^\mu T^{\lambda \nu} - x^{\nu}T^{\lambda \nu}$ is always conserved in that $\partial _{\lambda} M^{\lambda \mu \nu}=0$.
What I don't understand is that the claim is that the conservation of $M^{\lambda \mu \nu}$ results in the conservation of the total angular momentum tensor:
$J^{\mu \nu} = \int d^3x M^{0 \mu \nu}$
In essence, it is claimed that symmetry of stress energy tensor -> conservation of $M^{\lambda \mu \nu}$ -> Conservation of $J^{\mu \nu}$.
I don't see how this last step holds. I have tried the algebra, but I don't see how you can deduce anything about $\partial _{\mu} M^{0 \mu \nu}$, which you would need to vanish for $\partial _{\mu} J^{\mu \nu}$ to vanish i.e. for the angular momentum tensor to be conserved, based on $\partial _{\lambda} M^{\lambda \mu \nu}=0$ where $\lambda$ has not been set to 0, and is a sum over $\lambda$.