<oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:title>A geometric approach to finite rank unitary perturbations</dc:title>
<dc:creator>R. Douglas</dc:creator><dc:creator>Constanze Liaw</dc:creator>
<dc:subject>44A15</dc:subject><dc:subject>47A20</dc:subject><dc:subject>47A55Finite rank perturbations</dc:subject><dc:subject>rank one perturbations</dc:subject><dc:subject>dilation theory</dc:subject><dc:subject>normalized
Cauchy transform</dc:subject>
<dc:description>This paper concerns certain families of unitary operators, defined on a separable Hilbert space. Each family consists of all rank $n$ perturbations of a given completely nonunitary (cnu) contraction $T$ with defect indices $(n,n)$. We use the highly developed model theory of Sz.-Nagy and Foia\c s.

Namely, for fixed $n\in\mathbb{N}$, we consider a family of rank $n$ perturbations of $T$. Moreover, we also consider the analogous family of cnu contractions that arise as rank $n$ perturbations of $T$. We allow the corresponding characteristic operator function of $T$ to be non-inner.

We relate the unitary dilation of such a contraction to its rank $n$ unitary perturbations. Based on this construction, we prove that the spectra of the perturbed operators are purely singular if and only if the operator-valued characteristic function corresponding to the unperturbed operator is inner. In the case where $n=1$, the latter statement reduces to a well-known result in the theory of rank one perturbations. However, our method of proof via the theory of dilations extends to the case of arbitrary $n\in\mathbb{N}$.

We find a formula for the operator-valued characteristic functions corresponding to a family of related cnu contractions. In the case where $n=1$, for the characteristic function of the original contraction we obtain a simple expression involving the normalized Cauchy transform of a certain measure. An application of this representation then enables us to control the jump behavior of this normalized Cauchy transform &quot;across&quot; the unit circle.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2013</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2013.62.5028</dc:identifier>
<dc:source>10.1512/iumj.2013.62.5028</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 62 (2013) 333 - 354</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>