Let $H$ be a Hilbert space and $\phi \in H : \Vert\phi\Vert = 1$ fixed. Define the operator $T \in \mathcal L(H)$ by \begin{equation} Tx = \langle x, \phi\rangle \phi\,. \end{equation}
Determine the eigenvalues and the corresponding eigenvectors and -spaces of $T$.
A totally incomplete answer
The eigenvalues can be solved from the eigenvalue equation \begin{equation}\label{eq:eigenequation} Tx = \lambda x \quad\Leftrightarrow\quad (T - \lambda I) x = 0 \,, \tag{1} \end{equation} assuming $T - \lambda I$ is not injective. Also, if $(e_n)$ is a Schauder basis of $H$, after a bit of inner product manipulation $Tx$ can be written as \begin{equation} Tx = \langle x, \phi\rangle \phi = \left( \sum_n \langle x, e_n\rangle \langle e_n, \phi \rangle \right) \left( \sum_m \langle \phi, e_m\rangle e_m \right) = \left( \sum_n \langle x, e_n\rangle \langle e_n, \phi \rangle \left( \sum_m \langle \phi, e_m\rangle e_m \right)\right) \,. \end{equation} Now this is where I'm supposed to be using equation \eqref{eq:eigenequation}, I believe. This is because if we write $x$ using its Fourier series representation, we have \begin{equation} \lambda x = \lambda \sum_n \langle x, e_n\rangle e_n = \sum_n \lambda\langle x, e_n\rangle e_n, \end{equation} so setting \begin{equation} \left( \sum_n \langle x, e_n\rangle \langle e_n, \phi \rangle \left( \sum_m \langle \phi, e_m\rangle e_m \right)\right) = \sum_n \lambda\langle x, e_n\rangle e_n \end{equation} or \begin{equation} \left( \sum_n \langle x, e_n\rangle \langle e_n, \phi \rangle \left( \sum_m \langle \phi, e_m\rangle e_m \right)\right) - \sum_n \lambda\langle x, e_n\rangle e_n = 0 \end{equation} might allow us to solve for $\lambda$. But how the heck do I manipulate these indices so I end up with something I can use?
I tried opening the sums, but got nothing sensible.