<p>Assume that <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="62" /> </InlineMediaObject> <EquationSource Format="TEX">\((X,d,\mu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo>,</mo> <mi>d</mi> <mo>,</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is a metric space endowed with a non-negative Borel measure <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>μ</mi> </math></EquationSource> </InlineEquation> satisfying the doubling condition and the additional condition that <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="115" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu (B(x,r))\gtrsim r^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mrow> <mo stretchy="false">(</mo> <mi>B</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>r</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo>≳</mo> <msup> <mi>r</mi> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> for any <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq4.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="96" /> </InlineMediaObject> <EquationSource Format="TEX">\(x\in X, \,r&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>∈</mo> <mi>X</mi> <mo>,</mo> <mspace width="0.166667em" /> <mi>r</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and some <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq5.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(n\ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. Let <i>L</i> be a non-negative self-adjoint operator on <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq6.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^2(X,\mu )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo>,</mo> <mi>μ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. We assume that <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq7.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="TEX">\(e^{-tL}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>t</mi> <mi>L</mi> </mrow> </msup> </math></EquationSource> </InlineEquation> satisfies a Gaussian upper bound and the Schrödinger operator <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq8.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(e^{itL}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>e</mi> <mrow> <mi mathvariant="italic">itL</mi> </mrow> </msup> </math></EquationSource> </InlineEquation> satisfies an <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^1\rightarrow L^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>1</mn> </msup> <mo stretchy="false">→</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> decay estimate of the form <Equation ID="Equ22"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_Equ22.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="151" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \Vert e^{itL}\Vert _{L^1\rightarrow L^\infty } \lesssim |t|^{-\frac{n}{2}}. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mrow> <mo stretchy="false">‖</mo> </mrow> <msup> <mi>e</mi> <mrow> <mi mathvariant="italic">itL</mi> </mrow> </msup> <msub> <mrow> <mo stretchy="false">‖</mo> </mrow> <mrow> <msup> <mi>L</mi> <mn>1</mn> </msup> <mo stretchy="false">→</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> </mrow> </msub> <mo>≲</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>t</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mfrac> <mi>n</mi> <mn>2</mn> </mfrac> </mrow> </msup> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>Then for a general class of dispersive semigroup <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq10.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(e^{it\phi (L)}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>e</mi> <mrow> <mi>i</mi> <mi>t</mi> <mi>ϕ</mi> <mo stretchy="false">(</mo> <mi>L</mi> <mo stretchy="false">)</mo> </mrow> </msup> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq11.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="84" /> </InlineMediaObject> <EquationSource Format="TEX">\(\phi : {\mathbb {R}}^+ \rightarrow {\mathbb {R}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϕ</mi> <mo>:</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> </msup> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> is smooth, we establish a similar <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^1\rightarrow L^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>1</mn> </msup> <mo stretchy="false">→</mo> <msup> <mi>L</mi> <mi>∞</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> decay estimate by a suitable subordination formula connecting it with the Schrödinger operator <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2025_Article_IEq8.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(e^{itL}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>e</mi> <mrow> <mi mathvariant="italic">itL</mi> </mrow> </msup> </math></EquationSource> </InlineEquation>. As applications, we derive new Strichartz estimates for several dispersive equations related to Hermite operators, twisted Laplacians and Laguerre operators.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Decay Estimates for a Class of Semigroups Related to Self-adjoint Operators on Metric Measure Spaces

  • Guoxia Feng,
  • Manli Song,
  • Huoxiong Wu

摘要

Assume that \((X,d,\mu )\) ( X , d , μ ) is a metric space endowed with a non-negative Borel measure \(\mu \) μ satisfying the doubling condition and the additional condition that \(\mu (B(x,r))\gtrsim r^n\) μ ( B ( x , r ) ) r n for any \(x\in X, \,r>0\) x X , r > 0 and some \(n\ge 1\) n 1 . Let L be a non-negative self-adjoint operator on \(L^2(X,\mu )\) L 2 ( X , μ ) . We assume that \(e^{-tL}\) e - t L satisfies a Gaussian upper bound and the Schrödinger operator \(e^{itL}\) e itL satisfies an \(L^1\rightarrow L^\infty \) L 1 L decay estimate of the form \(\begin{aligned} \Vert e^{itL}\Vert _{L^1\rightarrow L^\infty } \lesssim |t|^{-\frac{n}{2}}. \end{aligned}\) e itL L 1 L | t | - n 2 . Then for a general class of dispersive semigroup \(e^{it\phi (L)}\) e i t ϕ ( L ) , where \(\phi : {\mathbb {R}}^+ \rightarrow {\mathbb {R}}\) ϕ : R + R is smooth, we establish a similar \(L^1\rightarrow L^\infty \) L 1 L decay estimate by a suitable subordination formula connecting it with the Schrödinger operator \(e^{itL}\) e itL . As applications, we derive new Strichartz estimates for several dispersive equations related to Hermite operators, twisted Laplacians and Laguerre operators.