<p>In this article, we prove null-controllability results for the heat equation associated to fractional Baouendi–Grushin operators <Equation ID="Equ53"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="28_2025_1069_Article_Equ53.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="239" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \partial _t u+\bigl (-\Delta _x-V(x)\Delta _y\bigr )^s u=\mathbb {1}_\Omega h \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mi>u</mi> <mo>+</mo> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">(</mo> </mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>x</mi> </msub> <mo>-</mo> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <msub> <mi mathvariant="normal">Δ</mi> <mi>y</mi> </msub> <msup> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">)</mo> </mrow> <mi>s</mi> </msup> <mi>u</mi> <mo>=</mo> <msub> <mn mathvariant="double-struck">1</mn> <mi mathvariant="normal">Ω</mi> </msub> <mi>h</mi> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <i>V</i> is a potential that satisfies some power growth conditions and the set <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="28_2025_1069_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation> is thick in some sense. This extends previously known results for potentials <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="28_2025_1069_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="92" /> </InlineMediaObject> <EquationSource Format="TEX">\(V(x)=|x|^{2k}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mn>2</mn> <mi>k</mi> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation>. To do so, we study Zhu-Zhuge’s spectral inequality for Schrödinger operators with power growth potentials, and give a precised quantitative form of it.</p>

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Null-controllability of the generalized Baouendi–Grushin heat like equations

  • Philippe Jaming,
  • Yunlei Wang

摘要

In this article, we prove null-controllability results for the heat equation associated to fractional Baouendi–Grushin operators \(\begin{aligned} \partial _t u+\bigl (-\Delta _x-V(x)\Delta _y\bigr )^s u=\mathbb {1}_\Omega h \end{aligned}\) t u + ( - Δ x - V ( x ) Δ y ) s u = 1 Ω h where V is a potential that satisfies some power growth conditions and the set \(\Omega \) Ω is thick in some sense. This extends previously known results for potentials \(V(x)=|x|^{2k}\) V ( x ) = | x | 2 k . To do so, we study Zhu-Zhuge’s spectral inequality for Schrödinger operators with power growth potentials, and give a precised quantitative form of it.