Since an eigenvector x {\displaystyle \mathbf {x} } of A {\displaystyle A} of eigenvalue λ 1 {\displaystyle \lambda _{1}} satisfies A x = λ 1 x {\textstyle A\mathbf {x} =\lambda _{1}\mathbf {x} } , i.e., ( A − λ 1 I ) x = 0 {\textstyle (A-\lambda _{1}I)\mathbf {x} =\mathbf {0} } , all we need to do is solve the following system.
By applying Gaussian elimination,
we obtain
Thus x 1 + 3 x 3 = 0 {\textstyle x_{1}+3x_{3}=0} and x 2 − 4 x 3 = 0 {\textstyle x_{2}-4x_{3}=0} ; in vector form we get