Unconditional bases of subspaces related to non-self-adjoint perturbations of self-adjoint operators
Abstract
Assume that $T$ is a self-adjoint operator on a Hilbert space $\mathcal{H}$ and that the spectrum of $T$ is confined in the union $\bigcup_{j\in J}\Delta_j$, $J\subseteq\mathbb{Z}$, of segments $\Delta_j=[\alpha_j, \beta_j]\subset\mathbb{R}$ such that $\alpha_{j+1}>\beta_j$ and $$ \inf_{j} \left(\alpha_{j+1}-\beta_j\right) = d > 0. $$ If $B$ is a bounded (in general non-self-adjoint) perturbation of $T$ with $\|B\|=:b<d/2$ then the spectrum of the perturbed operator $A=T+B$ lies in the union $\bigcup_{j\in J} U_{b}(\Delta_j)$ of the mutually disjoint closed $b$-neighborhoods $U_{b}(\Delta_j)$ of the segments $\Delta_j$ in $\mathbb{C}$. Let $Q_j$ be the Riesz projection onto the invariant subspace of $A$ corresponding to the part of the spectrum of $A$ lying in $U_{b}\left(\Delta_j\right)$, $j\in J$. Our main result is as follows: The subspaces $\mathcal{L}_j=Q_j(\mathcal H)$, $j\in J$, form an unconditional basis in the whole space $\mathcal H$.
- Publication:
-
arXiv e-prints
- Pub Date:
- January 2017
- DOI:
- arXiv:
- arXiv:1701.06296
- Bibcode:
- 2017arXiv170106296M
- Keywords:
-
- Mathematics - Spectral Theory;
- Mathematical Physics;
- Mathematics - Functional Analysis
- E-Print:
- Eurasian Mathematical Journal 8:1 (2017), 119-127 (http://mi.mathnet.ru/emj251)