<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(L=-{\Delta }_{{\mathbb {G}} }+V\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>L</mi> <mo>=</mo> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi mathvariant="double-struck">G</mi> </msub> <mo>+</mo> <mi>V</mi> </mrow> </math></EquationSource> </InlineEquation> be a Schrödinger operator on the stratified Lie group <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\({\mathbb {G}},\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="double-struck">G</mi> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> where <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\({\Delta }_{{\mathbb {G}} }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Δ</mi> <mi mathvariant="double-struck">G</mi> </msub> </math></EquationSource> </InlineEquation> is the sub-Laplacian and the nonnegative potential <i>V</i> belongs to the reverse Hölder class <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(B_{q}, q\ge {\mathcal {Q}}/2,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>B</mi> <mi>q</mi> </msub> <mo>,</mo> <mi>q</mi> <mo>≥</mo> <mi mathvariant="script">Q</mi> <mo stretchy="false">/</mo> <mn>2</mn> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> in which <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\({\mathcal {Q}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">Q</mi> </math></EquationSource> </InlineEquation> is the homogeneous dimension of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({\mathbb {G}}.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="double-struck">G</mi> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> In this article, we firstly study the fractional heat semigroups <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\{e^{-tL^{\alpha }}\}_{t&gt;0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">{</mo> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>t</mi> <msup> <mi>L</mi> <mi>α</mi> </msup> </mrow> </msup> <mo stretchy="false">}</mo> </mrow> <mrow> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </msub> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\alpha &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> associated with <i>L</i>. Subsequently, the regularities of the fractional heat semigroup is estimated with the use of the subordinative formula. Furthermore, in terms of application, we establish the <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(BMO_{L}^{\gamma }({\mathbb {G}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>B</mi> <mi>M</mi> <msubsup> <mi>O</mi> <mrow> <mi>L</mi> </mrow> <mi>γ</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">G</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>-boundedness of the maximal function and the Littlewood–Paley <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\({\mathfrak {g}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="fraktur">g</mi> </math></EquationSource> </InlineEquation>-functions related with the Schrödinger operator <i>L</i> by <i>T</i>1 theorem, respectively.</p>

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Boundedness of operators generated by fractional heat semigroups related to Schrödinger operators on stratified Lie groups via T1 theorem

  • Chuanhong Sun,
  • Pengtao Li,
  • Zengjian Lou

摘要

Let \(L=-{\Delta }_{{\mathbb {G}} }+V\) L = - Δ G + V be a Schrödinger operator on the stratified Lie group \({\mathbb {G}},\) G , where \({\Delta }_{{\mathbb {G}} }\) Δ G is the sub-Laplacian and the nonnegative potential V belongs to the reverse Hölder class \(B_{q}, q\ge {\mathcal {Q}}/2,\) B q , q Q / 2 , in which \({\mathcal {Q}}\) Q is the homogeneous dimension of \({\mathbb {G}}.\) G . In this article, we firstly study the fractional heat semigroups \(\{e^{-tL^{\alpha }}\}_{t>0}\) { e - t L α } t > 0 with \(\alpha >0\) α > 0 associated with L. Subsequently, the regularities of the fractional heat semigroup is estimated with the use of the subordinative formula. Furthermore, in terms of application, we establish the \(BMO_{L}^{\gamma }({\mathbb {G}})\) B M O L γ ( G ) -boundedness of the maximal function and the Littlewood–Paley \({\mathfrak {g}}\) g -functions related with the Schrödinger operator L by T1 theorem, respectively.