Problem: Let A=(1111111111111111). Compute all the eigenvalues and eigenvectors of A.
Attempt at solution: I found the eigenvalues by computing the characteristic polynomial. This gives me det after many steps. So the eigenvalues are \lambda_1 = 0 with multiplicity 3 and \lambda_2 = 4 with multiplicity 1.
Now I was trying to figure out what the eigenvectors are corresponding to these eigenvalues. Per definition we have Av = \lambda v, where v is an eigenvector with the corresponding eigenvalue. So I did for \lambda_2 = 4: \begin{align*} \begin{pmatrix} 1 & 1 & 1 & 1 \\ 1 & 1 & 1 & 1 \\ 1 & 1 & 1 & 1 \\ 1 & 1 & 1 & 1 \end{pmatrix} \begin{pmatrix} x_1 \\ x_2 \\ x_3 \\ x_4 \end{pmatrix} = 4 \begin{pmatrix} x_1 \\ x_2 \\ x_3 \\ x_4 \end{pmatrix} \end{align*} I think this is only possible when x_1 = x_2 = x_3 = x_4 = 1. So am I right in stating that all the eigenvectors corresponding to \lambda_2 are of the form t \begin{pmatrix} 1 \\ 1 \\ 1 \\ 1 \end{pmatrix} with t some number \neq 0? For \lambda_1 = 0, I'm not sure how to find the eigenvectors. The zero vector is never an eigenvector. This means x_1, x_2, x_3 and x_4 can be anything aslong as they add to zero?
Answer
You are right, and to show how this applies more generally, look at the eigenspace corresponding to the other eigenvalue, \lambda = 0. This has multiplicity 3, so we expect exactly 3 linearly independent vectors in this space. The main equation looks like A \vec{x} = 0 \vec{x} = \vec{0}, in other words,
\begin{pmatrix} 1 & 1 & 1 & 1 \\ 1 & 1 & 1 & 1 \\ 1 & 1 & 1 & 1 \\ 1 & 1 & 1 & 1 \end{pmatrix} \begin{pmatrix} x \\ y \\ z \\ w \end{pmatrix} = \begin{pmatrix} 0 \\ 0 \\ 0 \\ 0 \end{pmatrix}
It's not hard to see that we have 4 identical equations, so the only constraint is x + y + z + w = 0, so we define w = -x-y-z and any vector in the eigenspace now looks like
\begin{pmatrix} x \\ y \\ z \\ w \end{pmatrix} = \begin{pmatrix} x \\ y \\ z \\ -x-y-z \end{pmatrix} = x \begin{pmatrix} 1 \\ 0 \\ 0 \\ -1 \end{pmatrix} + y \begin{pmatrix} 0 \\ 1 \\ 0 \\ -1 \end{pmatrix} + z \begin{pmatrix} 0 \\ 0 \\ 1 \\ -1 \end{pmatrix}
and the three vectors which form the basis of the eigenspace are now specified.
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