These are called eigenvectors.
The scaling factors after transformation are called eigenvalues.
e.g. \( \begin{bmatrix} 2 \\ 1 \end{bmatrix} \) is an eigenvector of \( \begin{bmatrix} 5 & 0 \\ 2 & 1 \end{bmatrix} \) with the corresponding eigenvalue of 5.
This means if \( \vec{x} \) is an eigenvector of \( A \) w/ corresponding eigenvalue \( \lambda \), then:
\[ A\vec{x} = \lambda\vec{x} \]
Example
Is \( \vec{x} = \begin{bmatrix} -2 \\ 1 \end{bmatrix} \) an eigenvector of \( A = \begin{bmatrix} -1 & 4 \\ 3 & 3 \end{bmatrix} \)?
\[ A\vec{x} = \begin{bmatrix} -1 & 4 \\ 3 & 3 \end{bmatrix} \begin{bmatrix} -2 \\ 1 \end{bmatrix} = \begin{bmatrix} 6 \\ -3 \end{bmatrix} = -3 \begin{bmatrix} -2 \\ 1 \end{bmatrix} \]
Result: Yes, with \( \lambda = -3 \) and \( \vec{x} = \begin{bmatrix} -2 \\ 1 \end{bmatrix} \).