<p>Let <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">$ G $</EquationSource> </InlineEquation> be a&#xa0;convex domain with exactly one singular point <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">$ z_{s} $</EquationSource> </InlineEquation> of an analytic function <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="37" /> </InlineMediaObject> <EquationSource Format="TEX">$ Q(z) $</EquationSource> </InlineEquation>, symmetric with respect to this point.For large values of the modulus of the spectral parameter <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">$ \rho $</EquationSource> </InlineEquation>, we&#xa0;study the asymptotics of the transfer matrix <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">$ P $</EquationSource> </InlineEquation> of the Sturm–Liouville equation with potential <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq6.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">$ Q $</EquationSource> </InlineEquation> along an arbitrary curve lying in the domain <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">$ G $</EquationSource> </InlineEquation> and not passing through the point <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">$ z_{s} $</EquationSource> </InlineEquation>.Necessary and sufficient conditions are given under which the matrix <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">$ P $</EquationSource> </InlineEquation> is independent of the parameter <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">$ \rho $</EquationSource> </InlineEquation>, and its structure is described in this case.In all other cases, we prove that every entry of the transfer matrix is an entire function of <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">$ \rho $</EquationSource> </InlineEquation> of completely regular growth of order&#xa0;<InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11202_2025_1580_Article_IEq12.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">$ 1/2 $</EquationSource> </InlineEquation>, with the same piecewise trigonometric indicator and angular density of zeros.Formulas for these characteristics are obtained for three possible&#xa0;types.</p>

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Asymptotics of Solutions to the Sturm–Liouville Equation Along an Arbitrary Curve in a Neighborhood of a Symmetric Singular Point

  • A. A. Golubkov

摘要

Let $ G $ be a convex domain with exactly one singular point $ z_{s} $ of an analytic function $ Q(z) $ , symmetric with respect to this point.For large values of the modulus of the spectral parameter $ \rho $ , we study the asymptotics of the transfer matrix $ P $ of the Sturm–Liouville equation with potential $ Q $ along an arbitrary curve lying in the domain $ G $ and not passing through the point $ z_{s} $ .Necessary and sufficient conditions are given under which the matrix $ P $ is independent of the parameter $ \rho $ , and its structure is described in this case.In all other cases, we prove that every entry of the transfer matrix is an entire function of $ \rho $ of completely regular growth of order  $ 1/2 $ , with the same piecewise trigonometric indicator and angular density of zeros.Formulas for these characteristics are obtained for three possible types.