<p>We develop two functional models for closed isometric entire operators <i>V</i> with finite deficiency indices (<i>p</i>,&#xa0;<i>p</i>) acting in a separable Pontryagin space <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1729_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\mathcal {K}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">K</mi> </math></EquationSource> </InlineEquation>. In the first functional model it is shown that every such operator <i>V</i> is unitarily equivalent to a restriction <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1729_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(T^{{\mathfrak {E}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>T</mi> <mi mathvariant="fraktur">E</mi> </msup> </math></EquationSource> </InlineEquation> of the backward shift operator in the de Branges-Pontryagin space <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1729_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="37" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\mathcal {B}}}({{\mathfrak {E}}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">B</mi> <mo stretchy="false">(</mo> <mi mathvariant="fraktur">E</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1729_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\times 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>×</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> vector valued entire functions. The second functional model is used to parametrize a class of compressed coresolvents of extensions <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11785_2025_1729_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\widetilde{V}} }\)</EquationSource> <EquationSource Format="MATHML"><math> <mover accent="true"> <mi>V</mi> <mo stretchy="true">~</mo> </mover> </math></EquationSource> </InlineEquation> of <i>V</i> in terms of the range of a linear fractional transformation that is associated with the model. These results are applied to obtain a description of the set of solutions of an indefinite truncated trigonometric moment problem.</p>

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Entire Isometric Operators in de Branges–Pontryagin Spaces and Truncated Trigonometric Moment Problem

  • Volodymyr Derkach,
  • Harry Dym

摘要

We develop two functional models for closed isometric entire operators V with finite deficiency indices (pp) acting in a separable Pontryagin space \({{\mathcal {K}}}\) K . In the first functional model it is shown that every such operator V is unitarily equivalent to a restriction \(T^{{\mathfrak {E}}}\) T E of the backward shift operator in the de Branges-Pontryagin space \({{\mathcal {B}}}({{\mathfrak {E}}})\) B ( E ) of \(p\times 1\) p × 1 vector valued entire functions. The second functional model is used to parametrize a class of compressed coresolvents of extensions \({{\widetilde{V}} }\) V ~ of V in terms of the range of a linear fractional transformation that is associated with the model. These results are applied to obtain a description of the set of solutions of an indefinite truncated trigonometric moment problem.