so the e-vector corresponding to e-value \(\lambda = 1\) is
\[\vec{x} = \begin{bmatrix} r \\ 0 \end{bmatrix} = r \begin{bmatrix} 1 \\ 0 \end{bmatrix}\]
for simplicity, choose \(r=1\), so \(\vec{x} = \begin{bmatrix} 1 \\ 0 \end{bmatrix}\)
Similarly, for \(\lambda = 3\), \(\vec{x} = \begin{bmatrix} 1 \\ 1 \end{bmatrix}\)
7.4 Basic Theory of Systems of Eqs
if \(\vec{x}' = A\vec{x}\) and \(A\) is \(n \times n\), then there are \(n\) linearly independent solutions \(\vec{x}^{(1)}, \vec{x}^{(2)}, \dots, \vec{x}^{(n)}\)
(just like nth-order eq has \(n\) solutions)
then general solution is just a linearly combination of them:
\[\vec{x} = c_1 \vec{x}^{(1)} + c_2 \vec{x}^{(2)} + c_3 \vec{x}^{(3)} + \dots + c_n \vec{x}^{(n)}\]