Abstract
We consider the nonlocal Hénon-Gelfand–Liouville problem
for every \(s\in (0,1)\), \(a>0\) and \(n>2s\). We prove a monotonicity formula for solutions of the above equation using rescaling arguments. We apply this formula together with blow-down analysis arguments and technical integral estimates to establish non-existence of finite Morse index solutions when
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Acknowledgements
The research of the third author is partially supported by NSFC No.11801550 and NSFC No.11871470. The third author thanks Ali Hyder for many stimulating discussions.
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Appendix A
Appendix A
The purpose of this appendix is to provide necessary details for the proof of Proposition 2.5. First, we notice that the stability condition (1.3) can be extended to \(\overline{u}\). More precisely, if u is stable in \(\Omega \) then
for every \(\Phi \in C_c^\infty ({\overline{\mathbb {R}_+^{n+1}}})\) satisfying \(\varphi (\cdot ):=\Phi (\cdot ,0)\in C_c^\infty (\Omega )\). Indeed, if \(\overline{\varphi }\) is the s-harmonic extension of \(\varphi \), we have
Before giving the conclusion of Moser’s iteration, we present the following lemma which will be used in the later context.
Lemma A.1
Let \(e^{\alpha u}\in L^1( \Omega ) \) for some \(\Omega \subset \mathbb {R}^n\). Then \(t^{1-2s}e^{\alpha \overline{u}}\in L^1_{\mathrm {loc}}(\Omega \times [0, \infty ))\).
Proof
Let \(\Omega _0\Subset \Omega \) be fixed. Since \( u\in L_s(\mathbb {R}^n)\), we have for \(x\in \Omega _0\) and \(t\in (0,R)\)
where \(C \le g(x,t):=\int _{\Omega }P(X,y)dy\le 1\) for some positive constant C depending solely on R, \(\Omega _0\) and \(\Omega \). Therefore, by the Jensen’s inequality
where the constant C depends on \(R,~\Omega _0\) and \(\Omega \), but not on t. Hence,
This finishes the proof. \(\square \)
The following lemma is the main conclusion of this appendix and it is essential in the proof of Proposition 2.5.
Lemma A.2
Let \(u\in L_s(\mathbb {R}^n)\cap \dot{H}^s_{\mathrm {loc}}(\mathbb {R}^n)\) be a solution to (1.1). Assume that u is stable in \(\Omega \subseteq \mathbb {R}^n\). Let \(\Phi \in C_c^\infty ({{\overline{\mathbb {R}_+^{n+1}}}})\) be of the form \(\Phi (x,t) =\varphi (x)\eta (t)\) for some \(\varphi \in C_c^\infty (\Omega )\) and \(\eta \equiv 1\) on [0, 1]. Then for every \(0<\alpha <2\) we have
Proof
For \(k\in \mathbb {N}\) we set \(\overline{u}_k:=\min \{\overline{u},k\}\). Let \(u_k\) be the restriction of \(\overline{u}_k\) on \(\mathbb {R}^n\). It is straightforward to see that \(e^{2\alpha \overline{u}_k}\Phi ^2\) can be considered as a test function in (1.8). Therefore,
Now, we assume that \(t^{1-2s}e^{2(\alpha +\varepsilon )\overline{u}}\in L^1_{\mathrm {loc}}(\Omega \times [0,\infty ))\) for some \(\varepsilon >0\). Then by [28, Lemma 3.5], up to a subsequence, we have
Taking \(e^{\alpha \overline{u}_k} \Phi \) as a test function in the stability inequality (A.1) yields
where the last equality follows from integration by parts. Notice that the boundary term vanishes as \(\eta (t)=1\) on [0, 1]. Combining the prior estimates, we obtain
Concerning the last term in (A.4), one can notice that
Again, as \(\eta =1\) on [0, 1], the second term in the right-hand side of the above expression is identically zero for \(0\le t\le 1\). Therefore, Lemma A.1 yields
Thus,
provided \(\int _{\Omega }e^{2(\alpha +\varepsilon )u}dx<\infty .\) Now, choosing \(\alpha \in (0,\frac{1}{2})\) and \(0<\varepsilon <\frac{1}{2}-\alpha \) in the above estimate and then taking \(k\rightarrow \infty \) we conclude \(e^{(1+2\alpha )u}\in L^1_{\mathrm {loc}}(\Omega )\). By an iteration argument we conclude that \(e^{(1+2\alpha )u}\in L^1_{\mathrm {loc}}(\Omega )\) for every \(\alpha \in (0,2)\).
Now, send \(k\rightarrow \infty \) in (A.4) to get
And, take limit in (A.2) and (A.3) as \(k\rightarrow \infty \). Then, the proof of lemma follows immediately since the second term on the right-hand side of (A.2), when \(k\rightarrow \infty \), can be re-written as
Note that the boundary integral is zero as \(\eta =1\) on [0, 1]. This completes the proof. \(\square \)
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Fazly, M., Hu, Y. & Yang, W. On stable and finite Morse index solutions of the nonlocal Hénon-Gelfand–Liouville equation. Calc. Var. 60, 11 (2021). https://doi.org/10.1007/s00526-020-01874-7
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DOI: https://doi.org/10.1007/s00526-020-01874-7
Keywords
- Hénon-Gelfand–Liouville equation
- Fractional Laplacian
- Stable and finite Morse index solutions
- Monotonicity formula