Write
\begin{align*}
n^A &=
\begin{pmatrix}
n^0\\
n^1
\end{pmatrix},
&
k^A &=
\begin{pmatrix}
k^0\\
k^1
\end{pmatrix}.
\end{align*}
If
\begin{align*}
m^{AB} = n^A k^B,
\end{align*}
then the matrix representing ##m^{AB}##, with row index ##A## and column index##B##, is
\begin{align*}
[m^{AB}]
&=
\begin{pmatrix}
m^{00} & m^{01}\\
m^{10} & m^{11}
\end{pmatrix} \\
&=
\begin{pmatrix}
n^0 k^0 & n^0 k^1\\
n^1 k^0 & n^1 k^1
\end{pmatrix}.
\end{align*}
This is just the outer product: ##m = nk^T##.
Now ##m^{BA}## means the spinor obtained by interchanging the two indices. Since
\begin{align*}
m^{BA}=n^B k^A,
\end{align*}
its components, displayed again with row index ##A## and column index ##B##, are
\begin{align*}
[m^{BA}]
&=
\begin{pmatrix}
m^{00} & m^{10}\\
m^{01} & m^{11}
\end{pmatrix} \\
&=
\begin{pmatrix}
n^0 k^0 & n^1 k^0\\
n^0 k^1 & n^1 k^1
\end{pmatrix}.
\end{align*}
Thus,
\begin{align*}
[m^{BA}] = [m^{AB}]^T.
\end{align*}