<p>The main aim of this paper is to investigate the Lipschitz type continuity for the solutions of the invariant Laplacian Poisson equation <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="110" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _{\alpha } u(x)=\psi (x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mi>α</mi> </msub> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi>ψ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> in <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {B}}^{n}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq3.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="196" /> </InlineMediaObject> <EquationSource Format="TEX">\(u|_{{\mathbb {S}}^{n-1}}=\phi \in L^{\infty }\left( {\mathbb {S}}^{n-1}, {\mathbb {R}}^{n}\right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <msup> <mrow> <mi mathvariant="double-struck">S</mi> </mrow> <mrow> <mi>n</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> </msub> <mo>=</mo> <mi>ϕ</mi> <mo>∈</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> <mfenced close=")" open="("> <msup> <mrow> <mi mathvariant="double-struck">S</mi> </mrow> <mrow> <mi>n</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mo>,</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mfenced> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="115" /> </InlineMediaObject> <EquationSource Format="TEX">\(\psi \in L^{\infty }({\mathbb {B}}^{n},{\mathbb {R}}^{n})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ψ</mi> <mo>∈</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> <mo>,</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _{\alpha } \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation> is the invariant Laplacian operator in <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {R}}^{n}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq7.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(n\ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>. In order to reach this goal, firstly, we show that if <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq8.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="205" /> </InlineMediaObject> <EquationSource Format="TEX">\(u \in C^{2}\left( {\mathbb {B}}^{n}, {\mathbb {R}}^{n}\right) \cap C\left( \overline{{\mathbb {B}}^{n}},{\mathbb {R}}^{n}\right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>∈</mo> <msup> <mi>C</mi> <mn>2</mn> </msup> <mfenced close=")" open="("> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> <mo>,</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mfenced> <mo>∩</mo> <mi>C</mi> <mfenced close=")" open="("> <mover> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> <mo>¯</mo> </mover> <mo>,</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mfenced> </mrow> </math></EquationSource> </InlineEquation> is a solution to the above equation and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq9.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="124" /> </InlineMediaObject> <EquationSource Format="TEX">\( \psi (x) \left( 1-|x|^{2}\right) ^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ψ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mfenced close=")" open="("> <mn>1</mn> <mo>-</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> </mfenced> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> is integrable in <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {B}}^{n}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> </math></EquationSource> </InlineEquation>, then <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq11.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="133" /> </InlineMediaObject> <EquationSource Format="TEX">\(u=P_{\alpha }[\phi ]-G_{\alpha }[\psi ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>=</mo> <msub> <mi>P</mi> <mi>α</mi> </msub> <mrow> <mo stretchy="false">[</mo> <mi>ϕ</mi> <mo stretchy="false">]</mo> </mrow> <mo>-</mo> <msub> <mi>G</mi> <mi>α</mi> </msub> <mrow> <mo stretchy="false">[</mo> <mi>ψ</mi> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq12.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_{\alpha }[\phi ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>P</mi> <mi>α</mi> </msub> <mrow> <mo stretchy="false">[</mo> <mi>ϕ</mi> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq13.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(G_{\alpha }[\psi ]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>G</mi> <mi>α</mi> </msub> <mrow> <mo stretchy="false">[</mo> <mi>ψ</mi> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> denote the Poisson integral of <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq14.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\( \phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϕ</mi> </math></EquationSource> </InlineEquation> and Green integral of <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq15.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\( \psi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ψ</mi> </math></EquationSource> </InlineEquation> with respect to <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq16.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Delta _{\alpha }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation>, respectively. Secondly, we prove that if <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq17.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="327" /> </InlineMediaObject> <EquationSource Format="TEX">\(u=P_{\alpha }[\phi ]-G_{\alpha }[\psi ] \in C^{2}\left( {\mathbb {B}}^{n}, {\mathbb {R}}^{n}\right) \cap C\left( \overline{{\mathbb {B}}^{n}},{\mathbb {R}}^{n}\right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>=</mo> <msub> <mi>P</mi> <mi>α</mi> </msub> <mrow> <mo stretchy="false">[</mo> <mi>ϕ</mi> <mo stretchy="false">]</mo> </mrow> <mo>-</mo> <msub> <mi>G</mi> <mi>α</mi> </msub> <mrow> <mo stretchy="false">[</mo> <mi>ψ</mi> <mo stretchy="false">]</mo> </mrow> <mo>∈</mo> <msup> <mi>C</mi> <mn>2</mn> </msup> <mfenced close=")" open="("> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> <mo>,</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mfenced> <mo>∩</mo> <mi>C</mi> <mfenced close=")" open="("> <mover> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> <mo>¯</mo> </mover> <mo>,</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mfenced> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq9.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="124" /> </InlineMediaObject> <EquationSource Format="TEX">\( \psi (x) \left( 1-|x|^{2}\right) ^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ψ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mfenced close=")" open="("> <mn>1</mn> <mo>-</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> </mfenced> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> is integrable in <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {B}}^{n}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> </math></EquationSource> </InlineEquation>, then <i>u</i> is a solution to the above equation. Thirdly, we prove the main result of this paper. We show that if <InlineEquation ID="IEq20"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq20.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="74" /> </InlineMediaObject> <EquationSource Format="TEX">\(0&lt;\beta \le 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>β</mi> <mo>≤</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq21"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq21.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha &lt;1-\beta \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>&lt;</mo> <mn>1</mn> <mo>-</mo> <mi>β</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq22"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq17.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="327" /> </InlineMediaObject> <EquationSource Format="TEX">\(u=P_{\alpha }[\phi ]-G_{\alpha }[\psi ] \in C^{2}\left( {\mathbb {B}}^{n}, {\mathbb {R}}^{n}\right) \cap C\left( \overline{{\mathbb {B}}^{n}},{\mathbb {R}}^{n}\right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>=</mo> <msub> <mi>P</mi> <mi>α</mi> </msub> <mrow> <mo stretchy="false">[</mo> <mi>ϕ</mi> <mo stretchy="false">]</mo> </mrow> <mo>-</mo> <msub> <mi>G</mi> <mi>α</mi> </msub> <mrow> <mo stretchy="false">[</mo> <mi>ψ</mi> <mo stretchy="false">]</mo> </mrow> <mo>∈</mo> <msup> <mi>C</mi> <mn>2</mn> </msup> <mfenced close=")" open="("> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> <mo>,</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mfenced> <mo>∩</mo> <mi>C</mi> <mfenced close=")" open="("> <mover> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> <mo>¯</mo> </mover> <mo>,</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mfenced> </mrow> </math></EquationSource> </InlineEquation>, and if there are two non-negative constants <i>L</i>,&#xa0;<i>M</i> such that <InlineEquation ID="IEq23"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq23.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="186" /> </InlineMediaObject> <EquationSource Format="TEX">\(|\phi (\xi ) - \phi (\eta )| \le L |\xi - \eta |^{\beta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">|</mo> <mi>ϕ</mi> <mrow> <mo stretchy="false">(</mo> <mi>ξ</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mi>ϕ</mi> <mrow> <mo stretchy="false">(</mo> <mi>η</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> </mrow> <mo>≤</mo> <msup> <mrow> <mi>L</mi> <mo stretchy="false">|</mo> <mi>ξ</mi> <mo>-</mo> <mi>η</mi> <mo stretchy="false">|</mo> </mrow> <mi>β</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> for all <InlineEquation ID="IEq24"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq24.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="80" /> </InlineMediaObject> <EquationSource Format="TEX">\(\xi ,\eta \in {\mathbb {S}}^{n-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ξ</mi> <mo>,</mo> <mi>η</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">S</mi> </mrow> <mrow> <mi>n</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq25"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq25.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="162" /> </InlineMediaObject> <EquationSource Format="TEX">\(|\psi (x)| \le M (1 - |x|^2)^{\beta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">|</mo> <mi>ψ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> </mrow> <mo>≤</mo> <msup> <mrow> <mi>M</mi> <mo stretchy="false">(</mo> <mn>1</mn> <mo>-</mo> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <msup> <mrow> <mo stretchy="false">)</mo> </mrow> <mi>β</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> for all <InlineEquation ID="IEq26"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq26.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="TEX">\(x\in {\mathbb {B}}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>, then there exists a positive constant <i>N</i> such that for any <InlineEquation ID="IEq27"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq27.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="191" /> </InlineMediaObject> <EquationSource Format="TEX">\(|u(x) - u(y)| \le N |x - y|^{\beta } \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> </mrow> <mo>≤</mo> <msup> <mrow> <mi>N</mi> <mo stretchy="false">|</mo> <mi>x</mi> <mo>-</mo> <mi>y</mi> <mo stretchy="false">|</mo> </mrow> <mi>β</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> in <InlineEquation ID="IEq28"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq28.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{{\mathbb {B}}^n}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> <mo>¯</mo> </mover> </math></EquationSource> </InlineEquation>. Finally, we consider the local Lipschitz type continuity and we obtain a local spatial version of Privalov theorem for <InlineEquation ID="IEq29"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1934_Article_IEq29.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>-harmonic mappings.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Lipschitz type Continuity for Solutions of the Invariant Laplacian Poisson Equations

  • J. Chen,
  • Q. Li,
  • M. Mateljević,
  • N. Mutavdžić,
  • B. Purtić

摘要

The main aim of this paper is to investigate the Lipschitz type continuity for the solutions of the invariant Laplacian Poisson equation \(\Delta _{\alpha } u(x)=\psi (x)\) Δ α u ( x ) = ψ ( x ) in \({\mathbb {B}}^{n}\) B n , where \(u|_{{\mathbb {S}}^{n-1}}=\phi \in L^{\infty }\left( {\mathbb {S}}^{n-1}, {\mathbb {R}}^{n}\right) \) u | S n - 1 = ϕ L S n - 1 , R n , \(\psi \in L^{\infty }({\mathbb {B}}^{n},{\mathbb {R}}^{n})\) ψ L ( B n , R n ) and \(\Delta _{\alpha } \) Δ α is the invariant Laplacian operator in \({\mathbb {R}}^{n}\) R n for \(n\ge 3\) n 3 . In order to reach this goal, firstly, we show that if \(u \in C^{2}\left( {\mathbb {B}}^{n}, {\mathbb {R}}^{n}\right) \cap C\left( \overline{{\mathbb {B}}^{n}},{\mathbb {R}}^{n}\right) \) u C 2 B n , R n C B n ¯ , R n is a solution to the above equation and \( \psi (x) \left( 1-|x|^{2}\right) ^{-1}\) ψ ( x ) 1 - | x | 2 - 1 is integrable in \({\mathbb {B}}^{n}\) B n , then \(u=P_{\alpha }[\phi ]-G_{\alpha }[\psi ]\) u = P α [ ϕ ] - G α [ ψ ] , where \(P_{\alpha }[\phi ]\) P α [ ϕ ] and \(G_{\alpha }[\psi ]\) G α [ ψ ] denote the Poisson integral of \( \phi \) ϕ and Green integral of \( \psi \) ψ with respect to \(\Delta _{\alpha }\) Δ α , respectively. Secondly, we prove that if \(u=P_{\alpha }[\phi ]-G_{\alpha }[\psi ] \in C^{2}\left( {\mathbb {B}}^{n}, {\mathbb {R}}^{n}\right) \cap C\left( \overline{{\mathbb {B}}^{n}},{\mathbb {R}}^{n}\right) \) u = P α [ ϕ ] - G α [ ψ ] C 2 B n , R n C B n ¯ , R n and \( \psi (x) \left( 1-|x|^{2}\right) ^{-1}\) ψ ( x ) 1 - | x | 2 - 1 is integrable in \({\mathbb {B}}^{n}\) B n , then u is a solution to the above equation. Thirdly, we prove the main result of this paper. We show that if \(0<\beta \le 1\) 0 < β 1 , \(\alpha <1-\beta \) α < 1 - β , \(u=P_{\alpha }[\phi ]-G_{\alpha }[\psi ] \in C^{2}\left( {\mathbb {B}}^{n}, {\mathbb {R}}^{n}\right) \cap C\left( \overline{{\mathbb {B}}^{n}},{\mathbb {R}}^{n}\right) \) u = P α [ ϕ ] - G α [ ψ ] C 2 B n , R n C B n ¯ , R n , and if there are two non-negative constants LM such that \(|\phi (\xi ) - \phi (\eta )| \le L |\xi - \eta |^{\beta }\) | ϕ ( ξ ) - ϕ ( η ) | L | ξ - η | β for all \(\xi ,\eta \in {\mathbb {S}}^{n-1}\) ξ , η S n - 1 and \(|\psi (x)| \le M (1 - |x|^2)^{\beta }\) | ψ ( x ) | M ( 1 - | x | 2 ) β for all \(x\in {\mathbb {B}}^n\) x B n , then there exists a positive constant N such that for any \(|u(x) - u(y)| \le N |x - y|^{\beta } \) | u ( x ) - u ( y ) | N | x - y | β in \(\overline{{\mathbb {B}}^n}\) B n ¯ . Finally, we consider the local Lipschitz type continuity and we obtain a local spatial version of Privalov theorem for \(\alpha \) α -harmonic mappings.