AxiomOfChoice
- 531
- 1
(All that follows assumes we are talking about a self-adjoint operator A on a Hilbert space \mathscr H.) The first volume of Reed-Simon defines
<br /> \mathscr H_{\rm pp} = \left\{ \psi \in \mathscr H: \mu_\psi \text{ is pure point} \right\}.<br />
The book seems to take for granted that \mathscr H_{\rm pp} is a closed subspace of \mathscr H, but this is not at all obvious to me. Can someone please explain why this is the case? Thanks in advance!
I suppose I'd also like to know the following: Is there anything in \mathscr H_{\rm pp} that is not an eigenvector for A?
<br /> \mathscr H_{\rm pp} = \left\{ \psi \in \mathscr H: \mu_\psi \text{ is pure point} \right\}.<br />
The book seems to take for granted that \mathscr H_{\rm pp} is a closed subspace of \mathscr H, but this is not at all obvious to me. Can someone please explain why this is the case? Thanks in advance!
I suppose I'd also like to know the following: Is there anything in \mathscr H_{\rm pp} that is not an eigenvector for A?
Last edited: