<p>We analyze the main properties of the Bergman spaces of weak <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_714_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>- solutions for a biquaternionic Vekua equation of the form <Equation ID="Equ45"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_714_Article_Equ45.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="159" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} {\textbf{D}}w(x)-{\textbf{Q}}_Aw(x)=0 \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi mathvariant="bold">D</mi> <mi>w</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <msub> <mi mathvariant="bold">Q</mi> <mi>A</mi> </msub> <mi>w</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>0</mn> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>on bounded domains of <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_714_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {R}}^3\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </math></EquationSource> </InlineEquation>, where the operator <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_714_Article_IEq3.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\({\textbf{Q}}_A\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="bold">Q</mi> <mi>A</mi> </msub> </math></EquationSource> </InlineEquation> involves quaternionic conjugation and multiplications, both left and right, by essentially bounded functions. Properties such as completeness, separability, and reflexivity are shown. It is demonstrated that the solutions belonging to the Bergman spaces are locally Hölder continuous and that the evaluation maps are bounded in the <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_714_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>-norm. Consequently, for the case <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_714_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(p=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, we obtain a reproducing integral kernel and an explicit formula for the orthogonal projection onto the Bergman space. For <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_714_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="83" /> </InlineMediaObject> <EquationSource Format="TEX">\(1&lt;p&lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, the explicit form for the annihilator of the Bergman space in the dual <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_714_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_{p'}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <msup> <mi>p</mi> <mo>′</mo> </msup> </msub> </math></EquationSource> </InlineEquation> is presented, along with an orthogonal decomposition for <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_714_Article_IEq8.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>.</p>

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Bergman spaces and reproducing kernel for the biquaternionic Vekua equation

  • Víctor A. Vicente-Benítez

摘要

We analyze the main properties of the Bergman spaces of weak \(L_p\) L p - solutions for a biquaternionic Vekua equation of the form \(\begin{aligned} {\textbf{D}}w(x)-{\textbf{Q}}_Aw(x)=0 \end{aligned}\) D w ( x ) - Q A w ( x ) = 0 on bounded domains of \({\mathbb {R}}^3\) R 3 , where the operator \({\textbf{Q}}_A\) Q A involves quaternionic conjugation and multiplications, both left and right, by essentially bounded functions. Properties such as completeness, separability, and reflexivity are shown. It is demonstrated that the solutions belonging to the Bergman spaces are locally Hölder continuous and that the evaluation maps are bounded in the \(L_p\) L p -norm. Consequently, for the case \(p=2\) p = 2 , we obtain a reproducing integral kernel and an explicit formula for the orthogonal projection onto the Bergman space. For \(1<p<\infty \) 1 < p < , the explicit form for the annihilator of the Bergman space in the dual \(L_{p'}\) L p is presented, along with an orthogonal decomposition for \(L_2\) L 2 .