Abstract <p> We consider a radiation solution <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11503_2025_3255_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\psi\)</EquationSource> </InlineEquation> for the Helmholtz equation in an exterior domain in <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11503_2025_3255_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{R}^2\)</EquationSource> </InlineEquation>. We show that <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11503_2025_3255_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\psi\)</EquationSource> </InlineEquation> in the exterior domain is uniquely determined by its imaginary part <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11503_2025_3255_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(\operatorname{Im}(\psi)\)</EquationSource> </InlineEquation> on an interval of a line <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11503_2025_3255_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\(L\)</EquationSource> </InlineEquation> lying in the exterior domain. This result has a holographic prototype in the recent paper by Nair and Novikov (2025, J. Geom. Anal. 35, 4, 123). Some other curves for measurements, instead of the lines <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11503_2025_3255_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\(L\)</EquationSource> </InlineEquation>, are also considered. Applications to the Gelfand–Krein–Levitan inverse problem (from boundary values of the spectral measure in <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11503_2025_3255_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{R}^2\)</EquationSource> </InlineEquation>) and to passive imaging are also indicated. </p> <p> <b> DOI</b> 10.1134/S1061920825601077 </p>

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On the Reconstruction from the Imaginary Part for Radiation Solutions in Two Dimensions

  • A.V. Nair,
  • R.G. Novikov

摘要

Abstract

We consider a radiation solution \(\psi\) for the Helmholtz equation in an exterior domain in \(\mathbb{R}^2\) . We show that \(\psi\) in the exterior domain is uniquely determined by its imaginary part \(\operatorname{Im}(\psi)\) on an interval of a line \(L\) lying in the exterior domain. This result has a holographic prototype in the recent paper by Nair and Novikov (2025, J. Geom. Anal. 35, 4, 123). Some other curves for measurements, instead of the lines \(L\) , are also considered. Applications to the Gelfand–Krein–Levitan inverse problem (from boundary values of the spectral measure in \(\mathbb{R}^2\) ) and to passive imaging are also indicated.

DOI 10.1134/S1061920825601077