<p>In this article, we establish various characterizations of the parabolic Campanato space <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3108_Article_IEq1.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textrm{PC}_{\phi ,\gamma }^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mtext>PC</mtext> <mrow> <mi>ϕ</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mo>+</mo> </msubsup> </math></EquationSource> </InlineEquation> with time lag <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3108_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="69" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma \in (0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>γ</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, associated with an almost increasing function <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3108_Article_IEq3.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>, in terms of the parabolic John–Nirenberg inequality, the parabolic exponential integrability, the maximal medians, and the one-sided versions of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3108_Article_IEq1.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textrm{PC}_{\phi ,\gamma }^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mtext>PC</mtext> <mrow> <mi>ϕ</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mo>+</mo> </msubsup> </math></EquationSource> </InlineEquation>. These characterizations are then used to obtain four applications. Firstly, we characterize its null space. Secondly, based on a parabolic-shaped domain, we introduce the parabolic Lipschitz space with time lag and show its coincidence with <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3108_Article_IEq1.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textrm{PC}_{\phi ,\gamma }^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mtext>PC</mtext> <mrow> <mi>ϕ</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mo>+</mo> </msubsup> </math></EquationSource> </InlineEquation>. Thirdly, we demonstrate that classical Campanato spaces can be represented as <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3108_Article_IEq6.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="101" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textrm{PC}_{\phi ,\gamma }^{+}\cap \textrm{PC}_{\phi ,\gamma }^{-}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mtext>PC</mtext> <mrow> <mi>ϕ</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mo>+</mo> </msubsup> <mo>∩</mo> <msubsup> <mtext>PC</mtext> <mrow> <mi>ϕ</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mo>-</mo> </msubsup> </mrow> </math></EquationSource> </InlineEquation>. Fourthly, we quantify the distance from functions in the parabolic BMO space with time lag to <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3108_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>∞</mi> </msup> </math></EquationSource> </InlineEquation>. The main novelties lie in that the characterizations of <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3108_Article_IEq1.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textrm{PC}_{\phi ,\gamma }^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mtext>PC</mtext> <mrow> <mi>ϕ</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mo>+</mo> </msubsup> </math></EquationSource> </InlineEquation> require only the mild assumption that <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3108_Article_IEq3.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> is almost increasing, which is proved to be nearly optimal in some sense, and that, to establish the equivalence between parabolic Lipschitz spaces and <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3108_Article_IEq1.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textrm{PC}_{\phi ,\gamma }^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mtext>PC</mtext> <mrow> <mi>ϕ</mi> <mo>,</mo> <mi>γ</mi> </mrow> <mo>+</mo> </msubsup> </math></EquationSource> </InlineEquation>, we develop a new top/bottom edge anchored parabolic rectangle nesting method by fully exploiting the geometry of parabolic-shaped domains.</p>

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Optimal real-variable characterizations of parabolic Campanato spaces with time lag related to almost increasing functions

  • Weiyi Kong,
  • Dachun Yang,
  • Wen Yuan,
  • Chenfeng Zhu

摘要

In this article, we establish various characterizations of the parabolic Campanato space \(\textrm{PC}_{\phi ,\gamma }^{+}\) PC ϕ , γ + with time lag \(\gamma \in (0,1)\) γ ( 0 , 1 ) , associated with an almost increasing function \(\phi \) ϕ , in terms of the parabolic John–Nirenberg inequality, the parabolic exponential integrability, the maximal medians, and the one-sided versions of \(\textrm{PC}_{\phi ,\gamma }^{+}\) PC ϕ , γ + . These characterizations are then used to obtain four applications. Firstly, we characterize its null space. Secondly, based on a parabolic-shaped domain, we introduce the parabolic Lipschitz space with time lag and show its coincidence with \(\textrm{PC}_{\phi ,\gamma }^{+}\) PC ϕ , γ + . Thirdly, we demonstrate that classical Campanato spaces can be represented as \(\textrm{PC}_{\phi ,\gamma }^{+}\cap \textrm{PC}_{\phi ,\gamma }^{-}\) PC ϕ , γ + PC ϕ , γ - . Fourthly, we quantify the distance from functions in the parabolic BMO space with time lag to \(L^\infty \) L . The main novelties lie in that the characterizations of \(\textrm{PC}_{\phi ,\gamma }^{+}\) PC ϕ , γ + require only the mild assumption that \(\phi \) ϕ is almost increasing, which is proved to be nearly optimal in some sense, and that, to establish the equivalence between parabolic Lipschitz spaces and \(\textrm{PC}_{\phi ,\gamma }^{+}\) PC ϕ , γ + , we develop a new top/bottom edge anchored parabolic rectangle nesting method by fully exploiting the geometry of parabolic-shaped domains.