<p>This work investigates a mass-critical focusing inhomogeneous NLS with an inverse square potential. The paper proves the finite time blow-up of solutions for datum with negative energy without any radial or finite variance assumption. Moreover, the <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13661_2025_2053_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">$L^{2}$</EquationSource> </InlineEquation> concentration of nonglobal mass-critical solutions is established. This note complements (arXiv:<a href="http://arxiv.org/abs/2306.15210v1">2306.15210v1</a> [math.AP]) to the mass-critical regime and (Nonlinearity 35(8), <CitationRef CitationID="CR11">2022</CitationRef>) to the case with inverse square potential. The proof is based on a localized Virial type identity via the decaying factor <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13661_2025_2053_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mo stretchy="false">|</mo> <mi>x</mi> <msup> <mo stretchy="false">|</mo> <mrow> <mo>−</mo> <mi>b</mi> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">$|x|^{-b}$</EquationSource> </InlineEquation>, which gives a control, away from the origin, for the terms arising from the nonlinearity. Moreover, Hardy estimate is used to get the norm equivalence <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13661_2025_2053_Article_IEq3.gif" Format="GIF" Height="33" Rendition="HTML" Resolution="72" Type="Linedraw" Width="252" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">∥</mo> <mo>⋅</mo> <mo stretchy="false">∥</mo> </mrow> <mrow> <msup> <mover accent="true"> <mi>H</mi> <mo>˙</mo> </mover> <mn>1</mn> </msup> <mo stretchy="false">(</mo> <msup> <mi mathvariant="double-struck">R</mi> <mi>N</mi> </msup> <mo stretchy="false">)</mo> </mrow> </msub> <mo>∼</mo> <msub> <mrow> <mo stretchy="false">∥</mo> <msqrt> <mrow> <mo>−</mo> <mi mathvariant="normal">Δ</mi> <mo>+</mo> <mfrac> <mi>a</mi> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <msup> <mo stretchy="false">|</mo> <mn>2</mn> </msup> </mrow> </mfrac> </mrow> </msqrt> <mo>⋅</mo> <mo stretchy="false">∥</mo> </mrow> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mo stretchy="false">(</mo> <msup> <mi mathvariant="double-struck">R</mi> <mi>N</mi> </msup> <mo stretchy="false">)</mo> </mrow> </msub> </math></EquationSource> <EquationSource Format="TEX">$\|\cdot \|_{\dot{H}^{1}(\mathbb{R}^{N})}\sim \|\sqrt{-\Delta + \frac {a}{|x|^{2}}}\cdot \|_{L^{2}(\mathbb{R}^{N})}$</EquationSource> </InlineEquation>, which enables to handle the inverse square potential. This needs in particular the restrictions <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13661_2025_2053_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="48" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </math></EquationSource> <EquationSource Format="TEX">$N\geq 3$</EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13661_2025_2053_Article_IEq5.gif" Format="GIF" Height="27" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <mi>a</mi> <mo>&gt;</mo> <mo>−</mo> <mfrac> <msup> <mrow> <mo stretchy="false">(</mo> <mi>N</mi> <mo>−</mo> <mn>2</mn> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </msup> <mn>4</mn> </mfrac> </math></EquationSource> <EquationSource Format="TEX">$a&gt;-\frac{(N-2)^{2}}{4}$</EquationSource> </InlineEquation>. Furthermore, the <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13661_2025_2053_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">$L^{2}$</EquationSource> </InlineEquation> concentration is based on a compactness result in the spirit of (Int. Math. Res. Not. 46:2815-2828, (<CitationRef CitationID="CR13">2005</CitationRef>))</p>

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Mass-critical focusing inhomogeneous NLS with inverse square potential

  • Salah Boulaaras,
  • Tarek Saanouni

摘要

This work investigates a mass-critical focusing inhomogeneous NLS with an inverse square potential. The paper proves the finite time blow-up of solutions for datum with negative energy without any radial or finite variance assumption. Moreover, the L 2 $L^{2}$ concentration of nonglobal mass-critical solutions is established. This note complements (arXiv:2306.15210v1 [math.AP]) to the mass-critical regime and (Nonlinearity 35(8), 2022) to the case with inverse square potential. The proof is based on a localized Virial type identity via the decaying factor | x | b $|x|^{-b}$ , which gives a control, away from the origin, for the terms arising from the nonlinearity. Moreover, Hardy estimate is used to get the norm equivalence H ˙ 1 ( R N ) Δ + a | x | 2 L 2 ( R N ) $\|\cdot \|_{\dot{H}^{1}(\mathbb{R}^{N})}\sim \|\sqrt{-\Delta + \frac {a}{|x|^{2}}}\cdot \|_{L^{2}(\mathbb{R}^{N})}$ , which enables to handle the inverse square potential. This needs in particular the restrictions N 3 $N\geq 3$ and a > ( N 2 ) 2 4 $a>-\frac{(N-2)^{2}}{4}$ . Furthermore, the L 2 $L^{2}$ concentration is based on a compactness result in the spirit of (Int. Math. Res. Not. 46:2815-2828, (2005))