<p>We prove a family of dispersive estimates for the higher order Schrödinger equation <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="148" /> </InlineMediaObject> <EquationSource Format="TEX">\(iu_t=(-\Delta )^mu +Vu\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>i</mi> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>=</mo> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>m</mi> </msup> <mi>u</mi> <mo>+</mo> <mi>V</mi> <mi>u</mi> </mrow> </math></EquationSource> </InlineEquation> in <i>n</i> spatial dimensions, for <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(m\in \mathbb {N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq3.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(m&gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq4.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="104" /> </InlineMediaObject> <EquationSource Format="TEX">\(2m&lt;n&lt;4m\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mi>m</mi> <mo>&lt;</mo> <mi>n</mi> <mo>&lt;</mo> <mn>4</mn> <mi>m</mi> </mrow> </math></EquationSource> </InlineEquation>. Here <i>V</i> is a real-valued potential belonging to the closure of <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(C_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>C</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> functions with respect to the generalized Kato norm, which has critical scaling. Under standard assumptions on the spectrum, we show that <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq6.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="TEX">\(e^{-itH}P_{ac}(H)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>i</mi> <mi>t</mi> <mi>H</mi> </mrow> </msup> <msub> <mi>P</mi> <mrow> <mi mathvariant="italic">ac</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>H</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> satisfies a <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq7.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(|t|^{-\frac{n}{2m}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mo stretchy="false">|</mo> <mi>t</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mo>-</mo> <mfrac> <mi>n</mi> <mrow> <mn>2</mn> <mi>m</mi> </mrow> </mfrac> </mrow> </msup> </math></EquationSource> </InlineEquation> bound mapping <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq8.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^1\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>1</mn> </msup> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq9.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> by adapting a Wiener inversion theorem. We further show the lack of positive resonances for the operator <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq10.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="84" /> </InlineMediaObject> <EquationSource Format="TEX">\((-\Delta )^m +V\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>m</mi> </msup> <mo>+</mo> <mi>V</mi> </mrow> </math></EquationSource> </InlineEquation> and a family of dispersive estimates for operators of the form <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq11.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="147" /> </InlineMediaObject> <EquationSource Format="TEX">\(|H|^{\beta -\frac{n}{2m}}e^{-itH}P_{ac}(H)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>H</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>β</mi> <mo>-</mo> <mfrac> <mi>n</mi> <mrow> <mn>2</mn> <mi>m</mi> </mrow> </mfrac> </mrow> </msup> <msup> <mi>e</mi> <mrow> <mo>-</mo> <mi>i</mi> <mi>t</mi> <mi>H</mi> </mrow> </msup> <msub> <mi>P</mi> <mrow> <mi mathvariant="italic">ac</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>H</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2025_3146_Article_IEq12.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="75" /> </InlineMediaObject> <EquationSource Format="TEX">\(0&lt;\beta \le \frac{n}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>β</mi> <mo>≤</mo> <mfrac> <mi>n</mi> <mn>2</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. The results apply in both even and odd dimensions in the allowed range.</p>

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Dispersive estimates for higher order Schrödinger operators with scaling-critical potentials

  • M. Burak Erdoğan,
  • Michael Goldberg,
  • William R. Green

摘要

We prove a family of dispersive estimates for the higher order Schrödinger equation \(iu_t=(-\Delta )^mu +Vu\) i u t = ( - Δ ) m u + V u in n spatial dimensions, for \(m\in \mathbb {N}\) m N with \(m>1\) m > 1 and \(2m<n<4m\) 2 m < n < 4 m . Here V is a real-valued potential belonging to the closure of \(C_0\) C 0 functions with respect to the generalized Kato norm, which has critical scaling. Under standard assumptions on the spectrum, we show that \(e^{-itH}P_{ac}(H)\) e - i t H P ac ( H ) satisfies a \(|t|^{-\frac{n}{2m}}\) | t | - n 2 m bound mapping \(L^1\) L 1 to \(L^\infty \) L by adapting a Wiener inversion theorem. We further show the lack of positive resonances for the operator \((-\Delta )^m +V\) ( - Δ ) m + V and a family of dispersive estimates for operators of the form \(|H|^{\beta -\frac{n}{2m}}e^{-itH}P_{ac}(H)\) | H | β - n 2 m e - i t H P ac ( H ) for \(0<\beta \le \frac{n}{2}\) 0 < β n 2 . The results apply in both even and odd dimensions in the allowed range.