<p>In this paper, we study certain sectional structures of the <i>t</i>-scaled hypercomplex numbers <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{H}_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">H</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation> for a scale <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(t\in \mathbb{R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, including the quaternions <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="29" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{H}_{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">H</mi> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msub> </math></EquationSource> </InlineEquation>, and the split quaternions <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{H}_{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">H</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation>. For a fixed scale <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(t\in \mathbb{R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, by defining the collection <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{S}_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">S</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation> of certain pure-imaginary <i>t</i>-scaled hypercomplex number in <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{H}_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">H</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation>, we sectionize <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{H}_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">H</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation> from the imaginaries of <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{S}_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">S</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation>. We concentrate on a section <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq10.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{SH}_{I_{t}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">SH</mi> <msub> <mi>I</mi> <mi>t</mi> </msub> </msub> </math></EquationSource> </InlineEquation> for an arbitrarily fixed imaginary <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq11.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="TEX">\(I_{t}\in \mathbb{S}_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>I</mi> <mi>t</mi> </msub> <mo>∈</mo> <msub> <mi mathvariant="double-struck">S</mi> <mi>t</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, called the <i>t</i>-scaled section for <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq12.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(I_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>I</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation>. Differentiation theory on the section <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq10.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{SH}_{I_{t}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">SH</mi> <msub> <mi>I</mi> <mi>t</mi> </msub> </msub> </math></EquationSource> </InlineEquation> is studied in terms of that on <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{H}_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">H</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation> by regarding <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq10.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{SH}_{I_{t}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">SH</mi> <msub> <mi>I</mi> <mi>t</mi> </msub> </msub> </math></EquationSource> </InlineEquation> as a sub-structure of <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{H}_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">H</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation>. Also, some functional vector spaces induced by <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq17.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb{SH}}_{I_{t}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">SH</mi> <msub> <mi>I</mi> <mi>t</mi> </msub> </msub> </math></EquationSource> </InlineEquation> over the real field <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq18.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">R</mi> </math></EquationSource> </InlineEquation> are constructed and analyzed. And then an interesting type of operators on one of our vector spaces is considered. In particular, we are interested in Toeplitz-like operators. The main tool to do them is the isomorphic relation between <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq17.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb{SH}}_{I_{t}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">SH</mi> <msub> <mi>I</mi> <mi>t</mi> </msub> </msub> </math></EquationSource> </InlineEquation> and the <i>t</i>-scaled hyperbolics <InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq20.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb{D}_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">D</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation>, for “all” <InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq11.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="TEX">\(I_{t}\in \mathbb{S}_{t}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>I</mi> <mi>t</mi> </msub> <mo>∈</mo> <msub> <mi mathvariant="double-struck">S</mi> <mi>t</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, for any scale <InlineEquation ID="IEq22"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_951_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(t\in \mathbb{R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Differentiation and certain operators on scaled sectional hypercomplex numbers

  • Daniel Alpay,
  • Ilwoo Cho

摘要

In this paper, we study certain sectional structures of the t-scaled hypercomplex numbers \(\mathbb{H}_{t}\) H t for a scale \(t\in \mathbb{R}\) t R , including the quaternions \(\mathbb{H}_{-1}\) H - 1 , and the split quaternions \(\mathbb{H}_{1}\) H 1 . For a fixed scale \(t\in \mathbb{R}\) t R , by defining the collection \(\mathbb{S}_{t}\) S t of certain pure-imaginary t-scaled hypercomplex number in \(\mathbb{H}_{t}\) H t , we sectionize \(\mathbb{H}_{t}\) H t from the imaginaries of \(\mathbb{S}_{t}\) S t . We concentrate on a section \(\mathbb{SH}_{I_{t}}\) SH I t for an arbitrarily fixed imaginary \(I_{t}\in \mathbb{S}_{t}\) I t S t , called the t-scaled section for \(I_{t}\) I t . Differentiation theory on the section \(\mathbb{SH}_{I_{t}}\) SH I t is studied in terms of that on \(\mathbb{H}_{t}\) H t by regarding \(\mathbb{SH}_{I_{t}}\) SH I t as a sub-structure of \(\mathbb{H}_{t}\) H t . Also, some functional vector spaces induced by \({\mathbb{SH}}_{I_{t}}\) SH I t over the real field \(\mathbb{R}\) R are constructed and analyzed. And then an interesting type of operators on one of our vector spaces is considered. In particular, we are interested in Toeplitz-like operators. The main tool to do them is the isomorphic relation between \({\mathbb{SH}}_{I_{t}}\) SH I t and the t-scaled hyperbolics \(\mathbb{D}_{t}\) D t , for “all” \(I_{t}\in \mathbb{S}_{t}\) I t S t , for any scale \(t\in \mathbb{R}\) t R .