Left-invertibility of rank-one perturbations

preprint2022arXivOpen access

Abstract

For each isometry VV acting on some Hilbert space and a pair of vectors ff and gg in the same Hilbert space, we associate a nonnegative number c(V;f,g)c(V;f,g) defined by c(V;f,g)=(∥f∥2−∥V∗f∥2)∥g∥2+∣1+⟨V∗f,g⟩∣2. c(V; f,g) = (\|f\|^2 - \|V^*f\|^2) \|g\|^2 + |1 + \langle V^*f , g\rangle|^2. We prove that the rank-one perturbation V+f⊗gV + f \otimes g is left-invertible if and only if c(V;f,g)≠0. c(V;f,g) \neq 0. We also consider examples of rank-one perturbations of isometries that are shift on some Hilbert space of analytic functions. Here, shift refers to the operator of multiplication by the coordinate function zz. Finally, we examine D+f⊗gD + f \otimes g, where DD is a diagonal operator with nonzero diagonal entries and ff and gg are vectors with nonzero Fourier coefficients. We prove that D+f⊗gD + f\otimes g is left-invertible if and only if D+f⊗gD+f\otimes g is invertible.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.