<p>In this paper, <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_457_Article_IEq1.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p(\mathbb {R}^d,\gamma _\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mo>,</mo> <msub> <mi>γ</mi> <mi>∞</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>-boundedness properties for Littlewood–Paley g-functions involving time and spatial derivatives of Ornstein–Uhlenbeck semigroups are established. Here, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_457_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="25" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma _\infty\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>γ</mi> <mi>∞</mi> </msub> </math></EquationSource> </InlineEquation> denotes the invariant measure. To prove the strong type results for <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_457_Article_IEq3.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>, we use <i>R</i>-boundedness. The weak type (1,1) property is established by studying separately global and local operators defined for the Littlewood–Paley g-functions. By the way <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43034_2025_457_Article_IEq1.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p(\mathbb {R}^d,\gamma _\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> <mo>,</mo> <msub> <mi>γ</mi> <mi>∞</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>-boundedness properties for maximal and variation operators for Ornstein–Uhlenbeck semigroups are proved.</p>

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Littlewood–Paley functions associated with general Ornstein–Uhlenbeck semigroups

  • Víctor Almeida,
  • Jorge J. Betancor,
  • Juan C. Fariña,
  • Pablo Quijano,
  • Lourdes Rodríguez-Mesa

摘要

In this paper, \(L^p(\mathbb {R}^d,\gamma _\infty )\) L p ( R d , γ ) -boundedness properties for Littlewood–Paley g-functions involving time and spatial derivatives of Ornstein–Uhlenbeck semigroups are established. Here, \(\gamma _\infty\) γ denotes the invariant measure. To prove the strong type results for \(1<p< {\infty}\) 1 < p < , we use R-boundedness. The weak type (1,1) property is established by studying separately global and local operators defined for the Littlewood–Paley g-functions. By the way \(L^p(\mathbb {R}^d,\gamma _\infty )\) L p ( R d , γ ) -boundedness properties for maximal and variation operators for Ornstein–Uhlenbeck semigroups are proved.