<p>In this study, we explore biorthogonal nonuniform multiresolution analysis within Sobolev spaces, utilizing the framework of spectral pairs. For each <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\( j \in \mathbb {Z} \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>j</mi> <mo>∈</mo> <mi mathvariant="double-struck">Z</mi> </mrow> </math></EquationSource> </InlineEquation>, we consider the closed linear spans <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\( V_j \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>V</mi> <mi>j</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq3.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\( \tilde{V}_j \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover accent="true"> <mi>V</mi> <mo stretchy="false">~</mo> </mover> <mi>j</mi> </msub> </math></EquationSource> </InlineEquation>, which are generated by the sequences <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq4.gif" Format="GIF" Height="27" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\( \phi ^{(j)}_{j,\gamma } \)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>ϕ</mi> <mrow> <mi>j</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mrow> <mo stretchy="false">(</mo> <mi>j</mi> <mo stretchy="false">)</mo> </mrow> </msubsup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq5.gif" Format="GIF" Height="27" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\( \tilde{\phi }^{(j)}_{j,\gamma } \)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mover accent="true"> <mi>ϕ</mi> <mo stretchy="false">~</mo> </mover> <mrow> <mi>j</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mrow> <mo stretchy="false">(</mo> <mi>j</mi> <mo stretchy="false">)</mo> </mrow> </msubsup> </math></EquationSource> </InlineEquation>, respectively. The index <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq6.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\( \gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> is taken from the spectrum <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq7.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="146" /> </InlineMediaObject> <EquationSource Format="TEX">\( \Lambda _{r,N} = \left\{ 0, \frac{r}{N} \right\} + 2\mathbb {Z}, \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Λ</mi> <mrow> <mi>r</mi> <mo>,</mo> <mi>N</mi> </mrow> </msub> <mo>=</mo> <mfenced close="}" open="{"> <mn>0</mn> <mo>,</mo> <mfrac> <mi>r</mi> <mi>N</mi> </mfrac> </mfenced> <mo>+</mo> <mn>2</mn> <mi mathvariant="double-struck">Z</mi> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> where <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\( N \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>N</mi> </math></EquationSource> </InlineEquation> is a positive integer and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq9.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\( r \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>r</mi> </math></EquationSource> </InlineEquation> is an odd integer satisfying <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="116" /> </InlineMediaObject> <EquationSource Format="TEX">\( 1 \le r \le 2N - 1 \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>≤</mo> <mi>r</mi> <mo>≤</mo> <mn>2</mn> <mi>N</mi> <mo>-</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, with the constraint that <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq9.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\( r \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>r</mi> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10958_2025_7943_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\( N \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>N</mi> </math></EquationSource> </InlineEquation> are coprime. We establish the pre-Riesz condition for scaling functions within Sobolev spaces and provide the required and sufficient criteria for the translations of a single scaling function to construct Riesz bases. Furthermore, we demonstrate that, under mild constraints, the associated wavelets can form Riesz bases. Lastly, we examine the frame condition for nonuniform wavelets in Sobolev spaces, ensuring a rigorous mathematical foundation for their application.</p>

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NONUNIFORM BIORTHOGONAL WAVELETS IN SOBOLEV SPACES

  • Reena,
  • Vijay Kumar Yadav,
  • Raj Kumar,
  • Manish Chauhan

摘要

In this study, we explore biorthogonal nonuniform multiresolution analysis within Sobolev spaces, utilizing the framework of spectral pairs. For each \( j \in \mathbb {Z} \) j Z , we consider the closed linear spans \( V_j \) V j and \( \tilde{V}_j \) V ~ j , which are generated by the sequences \( \phi ^{(j)}_{j,\gamma } \) ϕ j , γ ( j ) and \( \tilde{\phi }^{(j)}_{j,\gamma } \) ϕ ~ j , γ ( j ) , respectively. The index \( \gamma \) γ is taken from the spectrum \( \Lambda _{r,N} = \left\{ 0, \frac{r}{N} \right\} + 2\mathbb {Z}, \) Λ r , N = 0 , r N + 2 Z , where \( N \) N is a positive integer and \( r \) r is an odd integer satisfying \( 1 \le r \le 2N - 1 \) 1 r 2 N - 1 , with the constraint that \( r \) r and \( N \) N are coprime. We establish the pre-Riesz condition for scaling functions within Sobolev spaces and provide the required and sufficient criteria for the translations of a single scaling function to construct Riesz bases. Furthermore, we demonstrate that, under mild constraints, the associated wavelets can form Riesz bases. Lastly, we examine the frame condition for nonuniform wavelets in Sobolev spaces, ensuring a rigorous mathematical foundation for their application.