(d) $\mathbf{L} = \mathbf{r} \times \mathbf{P} = \left| \begin{matrix}
\widehat{\mathbf{i}} & \widehat{\mathbf{j}} & \widehat{\mathbf{k}} \\
1 & 2 & - 1 \\
3 & 4 & - 2
\end{matrix} \right|\ $
$\mathbf{L} = \widehat{\mathbf{i}}( - 4 + 4) - \widehat{\mathbf{j}}( - 2 + 3) + \widehat{\mathbf{k}}(4 - 6) = - \widehat{\mathbf{j}} - 2\widehat{\mathbf{k}}$
$\mathbf{L}$ has components along $–y$ axis and $–z$ axis.
The angular momentum is in $y - z$ plane $ie$., perpendicular to $x$-axis.