<p>In this paper, pseudo-differential operators on <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="9_2025_2994_Article_IEq3.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {Z}^{n+1}_{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mi mathvariant="double-struck">Z</mi> </mrow> <mo>+</mo> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msubsup> </math></EquationSource> </InlineEquation> involving the Fourier Bessel transform are introduced and proved that these operators map the Schwartz space <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="9_2025_2994_Article_IEq4.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="TEX">\(S_{*}(\mathbb {Z}^{n+1}_{+})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mi>S</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> <mrow /> </mmultiscripts> <mrow> <mo stretchy="false">(</mo> <msubsup> <mrow> <mi mathvariant="double-struck">Z</mi> </mrow> <mo>+</mo> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msubsup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> into itself. Using this theory, we discussed the boundedness result of Friedrich’s operators on <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="9_2025_2994_Article_IEq5.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="66" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^{2}_{\alpha }(\mathbb {T}_{+}^{n+1})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>L</mi> <mi>α</mi> <mn>2</mn> </msubsup> <mrow> <mo stretchy="false">(</mo> <msubsup> <mi mathvariant="double-struck">T</mi> <mrow> <mo>+</mo> </mrow> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msubsup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>-type Sobolev space <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="9_2025_2994_Article_IEq6.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {H}}^{s,2}_{\alpha }(\mathbb {Z}_{+}^{n+1})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mrow> <mi mathvariant="script">H</mi> </mrow> <mi>α</mi> <mrow> <mi>s</mi> <mo>,</mo> <mn>2</mn> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <msubsup> <mi mathvariant="double-struck">Z</mi> <mrow> <mo>+</mo> </mrow> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msubsup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. These results are applied to get the solution of the heat equation on the frequency space <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="9_2025_2994_Article_IEq7.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {T}^{n+1}_{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mi mathvariant="double-struck">T</mi> </mrow> <mo>+</mo> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msubsup> </math></EquationSource> </InlineEquation>.</p>

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Pseudo-Differential Operators Involving the Fourier Bessel Transform on \(\mathbb {Z}_{+}^{n+1}\)

  • Mohd Sartaj,
  • Priyanka Balvant,
  • S. K. Upadhyay

摘要

In this paper, pseudo-differential operators on \(\mathbb {Z}^{n+1}_{+}\) Z + n + 1 involving the Fourier Bessel transform are introduced and proved that these operators map the Schwartz space \(S_{*}(\mathbb {Z}^{n+1}_{+})\) S ( Z + n + 1 ) into itself. Using this theory, we discussed the boundedness result of Friedrich’s operators on \(L^{2}_{\alpha }(\mathbb {T}_{+}^{n+1})\) L α 2 ( T + n + 1 ) -type Sobolev space \({\mathcal {H}}^{s,2}_{\alpha }(\mathbb {Z}_{+}^{n+1})\) H α s , 2 ( Z + n + 1 ) . These results are applied to get the solution of the heat equation on the frequency space \(\mathbb {T}^{n+1}_{+}\) T + n + 1 .