General Clark model for finite-rank perturbations

Liaw, Constanze; Treil, Sergei

doi:10.2140/apde.2019.12.449

Download this article
	For screen
	For printing

Recent Issues

The Journal

Submission Guidelines

Submission Form

Policies for Authors

Ethics Statement

ISSN: 1948-206X (e-only)

ISSN: 2157-5045 (print)

Author Index

To Appear

Other MSP Journals

This article is available for purchase or by subscription. See below.

General Clark model for finite-rank perturbations

Constanze Liaw and Sergei Treil

Vol. 12 (2019), No. 2, 449–492

DOI: 10.2140/apde.2019.12.449

Abstract

All unitary (contractive) perturbations of a given unitary operator $U$ by finite-rank- $d$ operators with fixed range can be parametrized by $d \times d$ unitary (contractive) matrices $Γ$ ; this generalizes unitary rank-one ( $d = 1$ ) perturbations, where the Aleksandrov–Clark family of unitary perturbations is parametrized by the scalars on the unit circle $T \subset ℂ$ .

For a strict contraction $Γ$ the resulting perturbed operator $T_{Γ}$ is (under the natural assumption about star cyclicity of the range) a completely nonunitary contraction, so it admits the functional model.

We investigate the Clark operator, i.e., a unitary operator that intertwines $T_{Γ}$ (written in the spectral representation of the nonperturbed operator $U$ ) and its model. We make no assumptions on the spectral type of the unitary operator $U$ ; an absolutely continuous spectrum may be present.

We first find a universal representation of the adjoint Clark operator in the coordinate-free Nikolski–Vasyunin functional model; the word “universal” means that it is valid in any transcription of the model. This representation can be considered to be a special version of the vector-valued Cauchy integral operator.

Combining the theory of singular integral operators with the theory of functional models, we derive from this abstract representation a concrete formula for the adjoint of the Clark operator in the Sz.-Nagy–Foiaş transcription. As in the scalar case, the adjoint Clark operator is given by a sum of two terms: one is given by the boundary values of the vector-valued Cauchy transform (postmultiplied by a matrix-valued function) and the second one is just the multiplication operator by a matrix-valued function.

Finally, we present formulas for the direct Clark operator in the Sz.-Nagy–Foiaş transcription.

PDF Access Denied

We have not been able to recognize your IP address 18.223.107.149 as that of a subscriber to this journal.
Online access to the content of recent issues is by subscription, or purchase of single articles.

Please contact your institution's librarian suggesting a subscription, for example by using our journal-recommendation form. Or, visit our subscription page for instructions on purchasing a subscription.

You may also contact us at contact@msp.org
or by using our contact form.

Or, you may purchase this single article for USD 40.00:

Keywords

finite-rank perturbations, Clark theory, dilation theory, functional model, normalized Cauchy transform

Mathematical Subject Classification 2010

Primary: 44A15, 47A20, 47A55

Milestones

Received: 20 November 2017

Revised: 17 April 2018

Accepted: 30 May 2018

Published: 14 August 2018

Authors

Constanze Liaw
Department of Mathematical Sciences University of Delaware Newark, DE United States	CASPER Baylor University Waco, TX United States

Sergei Treil
Department of Mathematics Brown University Providence, RI United States

Vol. 12, No. 2, 2019