<p>This article provides a revised version of some existing results in the literature for the quaternion Fourier transform (QFT) and quaternion wavelet transforms. The inner-product relation and its consequent formula for the continuous quaternion wavelet transform (CQWT) are derived in <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12215_2024_1180_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p ({\mathbb {R}}^{2}; {\mathbb {H}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mo>;</mo> <mi mathvariant="double-struck">H</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> space under the assumption that the admissible wavelet is complex-valued and has a real QFT. Furthermore, the characterization of quaternion Sobolev spaces <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12215_2024_1180_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\(H^{s}({\mathbb {R}}^{2}; {\mathbb {H}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mi>s</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mo>;</mo> <mi mathvariant="double-struck">H</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12215_2024_1180_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="82" /> </InlineMediaObject> <EquationSource Format="TEX">\(W^{m,p} (\Omega ; {\mathbb {H}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>W</mi> <mrow> <mi>m</mi> <mo>,</mo> <mi>p</mi> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo>;</mo> <mi mathvariant="double-struck">H</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, weighted quaternion Sobolev space <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12215_2024_1180_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="85" /> </InlineMediaObject> <EquationSource Format="TEX">\(W_{k}^{m,p} (\varvec{\Omega }; {\mathbb {H}} )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>W</mi> <mrow> <mi>k</mi> </mrow> <mrow> <mi>m</mi> <mo>,</mo> <mi>p</mi> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mrow> <mi mathvariant="bold">Ω</mi> </mrow> <mo>;</mo> <mi mathvariant="double-struck">H</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and generalized quaternion Sobolev space <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12215_2024_1180_Article_IEq5.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="73" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_{w}^{\omega } ({\mathbb {R}}^{2}; {\mathbb {H}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mrow> <mi>w</mi> </mrow> <mi>ω</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> <mo>;</mo> <mi mathvariant="double-struck">H</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, quaternion Besov space by means of the CQWT is presented. The CQWT is analysed within these function and distribution spaces, yielding novel findings regarding continuity and boundedness.</p>

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The continuous quaternion wavelet transform on distribution spaces

  • Drema Lhamu,
  • Aparna Das,
  • Sunil Kumar Singh,
  • Awniya Kumar

摘要

This article provides a revised version of some existing results in the literature for the quaternion Fourier transform (QFT) and quaternion wavelet transforms. The inner-product relation and its consequent formula for the continuous quaternion wavelet transform (CQWT) are derived in \(L^p ({\mathbb {R}}^{2}; {\mathbb {H}})\) L p ( R 2 ; H ) space under the assumption that the admissible wavelet is complex-valued and has a real QFT. Furthermore, the characterization of quaternion Sobolev spaces \(H^{s}({\mathbb {R}}^{2}; {\mathbb {H}})\) H s ( R 2 ; H ) and \(W^{m,p} (\Omega ; {\mathbb {H}})\) W m , p ( Ω ; H ) , weighted quaternion Sobolev space \(W_{k}^{m,p} (\varvec{\Omega }; {\mathbb {H}} )\) W k m , p ( Ω ; H ) and generalized quaternion Sobolev space \(H_{w}^{\omega } ({\mathbb {R}}^{2}; {\mathbb {H}})\) H w ω ( R 2 ; H ) , quaternion Besov space by means of the CQWT is presented. The CQWT is analysed within these function and distribution spaces, yielding novel findings regarding continuity and boundedness.