<p>In this manuscript, we focus on studying a family of viscosity solutions <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\((u_\varepsilon )_{\varepsilon &gt; 0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi>u</mi> <mi>ε</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mrow> <mi>ε</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </msub> </math></EquationSource> </InlineEquation> for a singular perturbation problem driven by the normalized <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(p(x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>-Laplacian operator <Equation ID="Equ48"> <EquationSource Format="TEX">\( \left\{ \begin{array}{rclcl} \Delta _{p_{\varepsilon } (x)}^{\textrm{N}} u_{\varepsilon }(x) &amp; = &amp; \zeta _{\varepsilon }\left( u_{\varepsilon }\right) + f_{\varepsilon }(x) &amp; {\text {in}} &amp; \Omega , \\ u_{\varepsilon }(x) &amp; = &amp; g(x) &amp; {\text {on}} &amp; \partial \Omega , \end{array} \right. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msubsup> <mi mathvariant="normal">Δ</mi> <mrow> <msub> <mi>p</mi> <mi>ε</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> <mtext>N</mtext> </msubsup> <msub> <mi>u</mi> <mi>ε</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> <mtd> <mo>=</mo> </mtd> <mtd columnalign="left"> <mrow> <msub> <mi>ζ</mi> <mi>ε</mi> </msub> <mfenced close=")" open="("> <msub> <mi>u</mi> <mi>ε</mi> </msub> </mfenced> <mo>+</mo> <msub> <mi>f</mi> <mi>ε</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> <mtd> <mi mathvariant="normal">in</mi> </mtd> <mtd columnalign="left"> <mrow> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <msub> <mi>u</mi> <mi>ε</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> <mtd> <mo>=</mo> </mtd> <mtd columnalign="left"> <mrow> <mi>g</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mtd> <mtd> <mi mathvariant="normal">on</mi> </mtd> <mtd columnalign="left"> <mrow> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>We establish that the solutions exhibit uniform bounds, local Lipschitz continuity, and non-degeneracy properties in a regular domain <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\Omega \subset {\mathbb {R}}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> with a sufficiently smooth boundary datum. As a consequence, we demonstrate that, up to a subsequence, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\( \lim _{j \rightarrow \infty } u_{\varepsilon _j} = u_0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mo movablelimits="true">lim</mo> <mrow> <mi>j</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </msub> <msub> <mi>u</mi> <msub> <mi>ε</mi> <mi>j</mi> </msub> </msub> <mo>=</mo> <msub> <mi>u</mi> <mn>0</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(u_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> is a viscosity solution to a one-phase Bernoulli-type free boundary problem, enjoying uniform and optimal Lipschitz bounds.</p>

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A singular perturbation problem governed by the normalized \(p(x)\)-Laplacian operator

  • João Vitor da Silva,
  • Víctor A. B. Viloria

摘要

In this manuscript, we focus on studying a family of viscosity solutions \((u_\varepsilon )_{\varepsilon > 0}\) ( u ε ) ε > 0 for a singular perturbation problem driven by the normalized \(p(x)\) p ( x ) -Laplacian operator \( \left\{ \begin{array}{rclcl} \Delta _{p_{\varepsilon } (x)}^{\textrm{N}} u_{\varepsilon }(x) & = & \zeta _{\varepsilon }\left( u_{\varepsilon }\right) + f_{\varepsilon }(x) & {\text {in}} & \Omega , \\ u_{\varepsilon }(x) & = & g(x) & {\text {on}} & \partial \Omega , \end{array} \right. \) Δ p ε ( x ) N u ε ( x ) = ζ ε u ε + f ε ( x ) in Ω , u ε ( x ) = g ( x ) on Ω , We establish that the solutions exhibit uniform bounds, local Lipschitz continuity, and non-degeneracy properties in a regular domain \(\Omega \subset {\mathbb {R}}^n\) Ω R n with a sufficiently smooth boundary datum. As a consequence, we demonstrate that, up to a subsequence, \( \lim _{j \rightarrow \infty } u_{\varepsilon _j} = u_0\) lim j u ε j = u 0 , where \(u_0\) u 0 is a viscosity solution to a one-phase Bernoulli-type free boundary problem, enjoying uniform and optimal Lipschitz bounds.