<p>We prove Sobolev-Poincaré and Poincaré inequalities in variable Lebesgue spaces <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(L^{p(\cdot )}(\Omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, with <InlineEquation ID="IEq2"> <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> a bounded John domain, with weaker regularity assumptions on the exponent <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\({p(\cdot )}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> that have been used previously. In particular, we require <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({p(\cdot )}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> to satisfy a new <i>boundary</i> <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\log \)</EquationSource> <EquationSource Format="MATHML"><math> <mo>log</mo> </math></EquationSource> </InlineEquation><i>-Hölder condition</i> that imposes some logarithmic decay on the oscillation of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({p(\cdot )}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> towards the boundary of the domain. Some control over the interior oscillation of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({p(\cdot )}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is also needed, but it is given by a very general condition that allows <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\({p(\cdot )}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> to be discontinuous at every point of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation>. Our results follows from a local-to-global argument based on the continuity of certain Hardy type operators. We provide examples that show that our boundary <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\log \)</EquationSource> <EquationSource Format="MATHML"><math> <mo>log</mo> </math></EquationSource> </InlineEquation>-Hölder condition is essentially necessary for our main results. The same examples are adapted to show that this condition is not sufficient for other related inequalities. Finally, we give an application to a Neumann problem for a degenerate <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\({p(\cdot )}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>-Laplacian.</p>

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Poincaré and Sobolev Inequalities with Variable Exponents and log-Hölder Continuity Only at the Boundary

  • David Cruz-Uribe OFS,
  • Fernando López-García,
  • Ignacio Ojea

摘要

We prove Sobolev-Poincaré and Poincaré inequalities in variable Lebesgue spaces \(L^{p(\cdot )}(\Omega )\) L p ( · ) ( Ω ) , with \(\Omega \subset {\mathbb {R}}^n\) Ω R n a bounded John domain, with weaker regularity assumptions on the exponent \({p(\cdot )}\) p ( · ) that have been used previously. In particular, we require \({p(\cdot )}\) p ( · ) to satisfy a new boundary \(\log \) log -Hölder condition that imposes some logarithmic decay on the oscillation of \({p(\cdot )}\) p ( · ) towards the boundary of the domain. Some control over the interior oscillation of \({p(\cdot )}\) p ( · ) is also needed, but it is given by a very general condition that allows \({p(\cdot )}\) p ( · ) to be discontinuous at every point of \(\Omega \) Ω . Our results follows from a local-to-global argument based on the continuity of certain Hardy type operators. We provide examples that show that our boundary \(\log \) log -Hölder condition is essentially necessary for our main results. The same examples are adapted to show that this condition is not sufficient for other related inequalities. Finally, we give an application to a Neumann problem for a degenerate \({p(\cdot )}\) p ( · ) -Laplacian.