<p>In this article we investigate an asymptotically critical problem involving the fractional Laplacian operator <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\((-\Delta _g)^s\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>g</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> </math></EquationSource> </InlineEquation> in a compact Riemannian <i>N</i>-manifold (<i>M</i>,&#xa0;<i>g</i>) as follows : <Equation ID="Equ114"> <EquationSource Format="TEX">\({\left\{ \begin{array}{ll}(-\Delta _g)^su+hu=u^{2_s^*-1\pm \epsilon ^s} &amp; \text {in} \ M \\ u&gt;0 &amp; \text {in} \ M\end{array}\right. }\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>g</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> <mi>u</mi> <mo>+</mo> <mi>h</mi> <mi>u</mi> <mo>=</mo> <msup> <mi>u</mi> <mrow> <msubsup> <mn>2</mn> <mi>s</mi> <mo>∗</mo> </msubsup> <mo>-</mo> <mn>1</mn> <mo>±</mo> <msup> <mi>ϵ</mi> <mi>s</mi> </msup> </mrow> </msup> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="4pt" /> <mi>M</mi> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="4pt" /> <mi>M</mi> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(2_s^*=\frac{2N}{N-2s}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mn>2</mn> <mi>s</mi> <mo>∗</mo> </msubsup> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>N</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> <mi>s</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(0&lt;s&lt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>s</mi> <mo>&lt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(N&gt;2s\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>&gt;</mo> <mn>2</mn> <mi>s</mi> </mrow> </math></EquationSource> </InlineEquation> with a small real parameter <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\epsilon \rightarrow 0^+\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϵ</mi> <mo stretchy="false">→</mo> <msup> <mn>0</mn> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>. We take <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(h:M\rightarrow \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>h</mi> <mo>:</mo> <mi>M</mi> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> initially a <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(C^1\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>C</mi> <mn>1</mn> </msup> </math></EquationSource> </InlineEquation>-function on <i>M</i>. In our work, we give an asymptotic estimate of the energy functional associated to the problem via rigorous estimates of norms of the bubble function concentrated at some point <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\xi _0\in M\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ξ</mi> <mn>0</mn> </msub> <mo>∈</mo> <mi>M</mi> </mrow> </math></EquationSource> </InlineEquation>. Using Lyapunov-Schmidt reduction, we then determine the condition on <i>h</i> such that the problem ensures a blow-up solution concentrated at <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\xi _0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ξ</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation>.</p>

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Blow up solutions of an asymptotically critical problem involving fractional Laplacian in compact Riemannian manifold

  • Arka Mukherjee,
  • Sweta Tiwari

摘要

In this article we investigate an asymptotically critical problem involving the fractional Laplacian operator \((-\Delta _g)^s\) ( - Δ g ) s in a compact Riemannian N-manifold (Mg) as follows : \({\left\{ \begin{array}{ll}(-\Delta _g)^su+hu=u^{2_s^*-1\pm \epsilon ^s} & \text {in} \ M \\ u>0 & \text {in} \ M\end{array}\right. }\) ( - Δ g ) s u + h u = u 2 s - 1 ± ϵ s in M u > 0 in M where \(2_s^*=\frac{2N}{N-2s}\) 2 s = 2 N N - 2 s with \(0<s<1\) 0 < s < 1 and \(N>2s\) N > 2 s with a small real parameter \(\epsilon \rightarrow 0^+\) ϵ 0 + . We take \(h:M\rightarrow \mathbb {R}\) h : M R initially a \(C^1\) C 1 -function on M. In our work, we give an asymptotic estimate of the energy functional associated to the problem via rigorous estimates of norms of the bubble function concentrated at some point \(\xi _0\in M\) ξ 0 M . Using Lyapunov-Schmidt reduction, we then determine the condition on h such that the problem ensures a blow-up solution concentrated at \(\xi _0\) ξ 0 .