<p>Let <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {L}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">L</mi> </math></EquationSource> </InlineEquation> be a Schrödinger operator and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {V}_\varrho (e^{-t\mathcal {L}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">V</mi> <mi>ϱ</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>t</mi> <mi mathvariant="script">L</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> be the variation operator of heat semigroup associated to <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {L}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">L</mi> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varrho &gt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϱ</mi> <mo>&gt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>. In this paper, we first obtain the quantitative weighted <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation> bounds for <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {V}_\varrho (e^{-t\mathcal {L}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">V</mi> <mi>ϱ</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>t</mi> <mi mathvariant="script">L</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with a class of weights related to critical radius functions, which contains the classical Muckenhoupt weights as a proper subset. Next, a new bump condition, which is weaker than the classical bump condition, is given for two-weight inequality of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {V}_\varrho (e^{-t\mathcal {L}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">V</mi> <mi>ϱ</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>t</mi> <mi mathvariant="script">L</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, and the weighted mixed weak type inequality corresponding to Sawyer’s conjecture for <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {V}_\varrho (e^{-t\mathcal {L}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">V</mi> <mi>ϱ</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>t</mi> <mi mathvariant="script">L</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is obtained. Furthermore, the quantitative restricted weak type (<i>p</i>,&#xa0;<i>p</i>) bounds for <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {V}_\varrho (e^{-t\mathcal {L}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">V</mi> <mi>ϱ</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>t</mi> <mi mathvariant="script">L</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> are also given with a new class of weights <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq10.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\(A_{p}^{\rho ,\theta ,\mathcal {R}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mrow> <mi>p</mi> </mrow> <mrow> <mi>ρ</mi> <mo>,</mo> <mi>θ</mi> <mo>,</mo> <mi mathvariant="script">R</mi> </mrow> </msubsup> </math></EquationSource> </InlineEquation>, which is larger than the classical <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq11.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="TEX">\(A_{p}^{\mathcal {R}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mrow> <mi>p</mi> </mrow> <mi mathvariant="script">R</mi> </msubsup> </math></EquationSource> </InlineEquation> weights. Meanwhile, several characterizations of <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41_2025_10166_Article_IEq12.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\(A_{p,q,\alpha }^{\rho ,\theta ,\mathcal {R}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo>,</mo> <mi>α</mi> </mrow> <mrow> <mi>ρ</mi> <mo>,</mo> <mi>θ</mi> <mo>,</mo> <mi mathvariant="script">R</mi> </mrow> </msubsup> </math></EquationSource> </InlineEquation> in terms of restricted weak type estimates of maximal operators are established.</p>

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Weighted Variational Inequalities for Heat Semigroups Associated with Schrödinger Operators Related to Critical Radius Functions

  • Yongming Wen,
  • Huoxiong Wu

摘要

Let \(\mathcal {L}\) L be a Schrödinger operator and \(\mathcal {V}_\varrho (e^{-t\mathcal {L}})\) V ϱ ( e - t L ) be the variation operator of heat semigroup associated to \(\mathcal {L}\) L with \(\varrho >2\) ϱ > 2 . In this paper, we first obtain the quantitative weighted \(L^p\) L p bounds for \(\mathcal {V}_\varrho (e^{-t\mathcal {L}})\) V ϱ ( e - t L ) with a class of weights related to critical radius functions, which contains the classical Muckenhoupt weights as a proper subset. Next, a new bump condition, which is weaker than the classical bump condition, is given for two-weight inequality of \(\mathcal {V}_\varrho (e^{-t\mathcal {L}})\) V ϱ ( e - t L ) , and the weighted mixed weak type inequality corresponding to Sawyer’s conjecture for \(\mathcal {V}_\varrho (e^{-t\mathcal {L}})\) V ϱ ( e - t L ) is obtained. Furthermore, the quantitative restricted weak type (pp) bounds for \(\mathcal {V}_\varrho (e^{-t\mathcal {L}})\) V ϱ ( e - t L ) are also given with a new class of weights \(A_{p}^{\rho ,\theta ,\mathcal {R}}\) A p ρ , θ , R , which is larger than the classical \(A_{p}^{\mathcal {R}}\) A p R weights. Meanwhile, several characterizations of \(A_{p,q,\alpha }^{\rho ,\theta ,\mathcal {R}}\) A p , q , α ρ , θ , R in terms of restricted weak type estimates of maximal operators are established.