<p>In this paper, we examine the following quasilinear Schrödinger equation <Equation ID="Equ42"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1857_Article_Equ42.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="343" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} -\Delta u-\Delta \left( u^{2}\right) u = \left( |x|^{\mu -n}*|u|^q\right) |u|^{q-2}u \text{ in } {\mathbb {R}}^{n}, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mfenced close=")" open="("> <msup> <mi>u</mi> <mn>2</mn> </msup> </mfenced> <mi>u</mi> <mo>=</mo> <mfenced close=")" open="("> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>μ</mi> <mo>-</mo> <mi>n</mi> </mrow> </msup> <mrow /> <mo>∗</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mi>q</mi> </msup> </mfenced> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1857_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="84" /> </InlineMediaObject> <EquationSource Format="TEX">\(q&gt;3+\sqrt{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>&gt;</mo> <mn>3</mn> <mo>+</mo> <msqrt> <mn>2</mn> </msqrt> </mrow> </math></EquationSource> </InlineEquation>. Under certain appropriate assumptions on <i>n</i> and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1857_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>, we establish a Liouville type theorem for the class of stable bounded sign-changing solutions to this problem.</p>

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Stable Solutions to Quasilinear Schrödinger Equations of Choquard Type

  • Belgacem Rahal

摘要

In this paper, we examine the following quasilinear Schrödinger equation \(\begin{aligned} -\Delta u-\Delta \left( u^{2}\right) u = \left( |x|^{\mu -n}*|u|^q\right) |u|^{q-2}u \text{ in } {\mathbb {R}}^{n}, \end{aligned}\) - Δ u - Δ u 2 u = | x | μ - n | u | q | u | q - 2 u in R n , where \(q>3+\sqrt{2}\) q > 3 + 2 . Under certain appropriate assumptions on n and \(\mu \) μ , we establish a Liouville type theorem for the class of stable bounded sign-changing solutions to this problem.