I'm trying to do some exercises about the manipulations of the indexes. I have the tensor $X^{\mu\nu}$ represented by the following matrix $$[X^{\mu\nu}] = [X] = \begin{pmatrix} 2 & 3 & 1 & 0 \\ 1 & 1 & 2 & 0 \\ 0 & 1 & 1 & 3 \\ 1 & 2 & 3 & 0 \end{pmatrix}$$
I have to calculate $X^{\mu}_{\phantom{a}\nu}$ so I understodood that
$$X^{\mu}_{\phantom{a}\nu}= X^{\mu\sigma}\eta_{\sigma\nu} = \sum_{k=0}^3 X^{\mu k}\eta_{k \nu}$$
The above object if expanded reads
$$X^{\mu 0}\eta_{0 \nu} + X^{\mu 1} \eta_{1 \nu} + \ldots$$
But the metric tensor $\eta_{\mu \nu} = diag(1, -1, -1, -1)$ has nonzero components only on the diagonal, hence I'd get
$$X^{\mu 0} \eta_{00} + \ldots $$
hence
$$X^{\mu 0} - X^{\mu 1} - X^{\mu 2} - X^{\mu 3}$$
The notation now makes me rather confused because $X^{\mu 0}$ is what? An object from $X^{\mu \nu}$ where the components $\mu$ are the first term of each row, since the column is the $0$-th one and reains fixed, that is
$$X^{\mu 0} = \begin{pmatrix} 2 \\ 1 \\ 0 \\ 1 \end{pmatrix}$$
If this holds for the other objects too, then what I am doing is summing four $4\times 1$ matrices, and I would get a $4\times 1$ matrix, not a $4\times 4 $ matrix in the end.
I am not understanding this...