For arbitrary tensors $\mathbf{A}$ and $\mathbf{B}$, does this commutativity relation for the tensor components always hold? Does it hold for dummy indices?
\begin{equation} {A^{\mu_1...\mu_n}}_{\nu_1...\nu_m}{B^{\alpha_1...\alpha_j}}_{\beta_1...\beta_k} = {B^{\alpha_1...\alpha_j}}_{\beta_1...\beta_k}{A^{\mu_1...\mu_n}}_{\nu_1...\nu_m} \end{equation}
If not, how would I prove that? If it holds for some tensors, how would I check? If always, is there an easy proof of this?
I’ve tried to find this elsewhere but am either searching for the wrong terms or not finding anything.
These $A^{\mu_1 ... \mu_n}_{\nu_1 ... \nu_m}$ and $B^{\alpha_1 ... \alpha_j}_{\beta_1 ... \beta_k}$ are just numbers, so they commute, as elements of your field. It's the same as writing $\vec{y} = M\vec{x} \rightarrow y_i = \sum M_{ij}x_j = \sum x_j M_{ij}$.