For the Eigenvalue,\({\lambda _i}\), matrix A satisfies the system of equations\(\left( {A - {\lambda _i}} \right){\rm{x}} = {\rm{0}}\).
For the Eigenvector, \(\lambda = 4 + 3i\), the system \(\left( {A - \lambda I} \right)\)is solved as follows:
\(\begin{aligned}{}A - \left( {4 + 3i} \right)I &= \left( {\begin{aligned}{}4&{}&3\\{ - 3}&{}&{\,\,4}\end{aligned}} \right) - \left( {4 + 3i} \right)\left( {\begin{aligned}{}1&{}&0\\{\,0}&{}&1\end{aligned}} \right)\\ &= \left( {\begin{aligned}{}{ - 3i}&{}&3\\{ - 3}&{}7{ - 3i}\end{aligned}} \right)\end{aligned}\)
The system of equations \(\left( {A - \lambda I} \right)x = 0\)gives the following equations:
\(\begin{aligned}{}\left( {\begin{aligned}{}{ - 3i}&{}&3\\{ - 3}&{}&{ - 3i}\end{aligned}} \right) &= 0\\\left( { - 3i} \right){x_1} + 3{x_2} &= 0\\ - 3{x_1} + \left( { - 3i} \right){x_2} &= 0\end{aligned}\)
Both the equations are equivalent to the equation, \({x_1} = - i{x_2}\), in which \({x_2}\) the variable is free. So, the general solution is \({x_1}\left( \begin{aligned}{} - i\\\,\,1\end{aligned} \right)\) and the corresponding Eigenvector is \({{\bf{v}}_1} = \left( \begin{aligned}{} - i\\\,\,1\end{aligned} \right)\).
For the Eigenvector, \(\lambda = 4 - 3i\), the system \(\left( {A - \lambda I} \right)\) is solved as follows:
\(\begin{aligned}{}A - \left( {4 - 3i} \right)I &= \left( {\begin{aligned}{}4&{}&3\\{ - 3}&{}&{\,\,4}\end{aligned}} \right) - \left( {4 - 3i} \right)\left( {\begin{aligned}{}1&{}&0\\{\,0}&{}&1\end{aligned}} \right)\\ &= \left( {\begin{aligned}{}{3i}&{}&3\\{ - 3}&{}&{3i}\end{aligned}} \right)\end{aligned}\)
The system of equations \(\left( {A - \lambda I} \right)x = 0\)gives the following equations:
\(\begin{aligned}{}\left( {\begin{aligned}{}{3i}&{}&3\\{ - 3}&{}&{3i}\end{aligned}} \right) &= 0\\3i{x_1} + 3{x_2} &= 0\\ - 3{x_1} + 3i{x_2} &= 0\end{aligned}\)
Both the equations are equivalent to the equation, \({x_1} = i{x_2}\), in which \({x_2}\) the variable is free. So, the general solution is \({x_2}\left( \begin{aligned}{}i\\1\end{aligned} \right)\) and the corresponding Eigenvector is \({{\bf{v}}_2} = \left( \begin{aligned}{}i\\1\end{aligned} \right)\).