Abstract
Let \((X, g^+)\) be an asymptotically hyperbolic manifold and \((M, [\hat{h}])\) be its conformal infinity. We construct positive clustered solutions to low-order perturbations of \(\gamma \)-Yamabe equations (\(0< \gamma < 1\)) on \((M, \hat{h})\), which are slightly supercritical, under certain geometric and dimensional assumptions. These solutions certainly exhibit non-isolated blow-up.
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Notes
The existence and uniqueness of the solution \(U \in H^{1,2}(X; \rho ^{1-2\gamma })\) for any given function \(g \in L^{p+1}(M)\) is guaranteed by the definition of the *-norm in (2.10) and the Riesz representation theorem. Also, [10, Lemma 3.3] implies that if \(g \in L^{q_{\epsilon }/(p+\epsilon )}(M)\), then \(u = U|_M \in L^{q_{\epsilon }}(M)\).
By (2.8), it holds that \(\delta ^{2\gamma } \sim \epsilon \), \(\delta ^{(n-2\gamma ) (\alpha -\beta )} \sim \epsilon ^{1 + {n-4\gamma \over \gamma (n-2\gamma +2)}}\) and \(\delta ^2 \sim \epsilon ^{1 \over \gamma }\).
The arguments in [25, Section 2] involving the Moser iteration technique also work in our setting, see [18, Section 3]. Also, in order to take advantage of the regularity theory, we need that the value of \(\sup _{\epsilon > 0} \Vert \Phi _{\ell \epsilon }^{p-1+\epsilon }\Vert _{L^{n/(2\gamma )}(M \setminus B_{\hat{h}}(\xi _0, r))}\) is sufficiently small for a fixed radius \(r > 0\), which is true owing to our choice of \(q_{\epsilon }\) in (2.11).
Once it is proved, even though the maximization argument does not work, we may apply the general critical point result of Thizy and Vétois [46, Lemma A.1].
Precisely, \(\mathcal {M}_0 > 0\) if \(n \ge 4\) for \(\gamma \in (\sqrt{5/11}, 1)\), \(n \ge 5\) for \(\gamma \in (1/2, 1)\), \(n \ge 6\) for \(\gamma \in (\sqrt{1/19}, 1)\) and \(n \ge 7\) for any \(\gamma \in (0,1)\). Observe that \(\mathcal {M}_0\) is the quantity that already appeared in [29, Corollary 2.7].
Here \(\zeta > 0\) is an arbitrary number in the nonempty interval \(((2\gamma n-4\gamma ^2-4)/(n-2\gamma +2), 2\gamma ]\) such that \(n > 2+2\gamma +\zeta \) (cf. Proof of Corollary 3.7 (1)).
The second integral in the parenthesis is \(O(\epsilon ^{1/\gamma })\) if \(n \ge 4\).
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Acknowledgements
Part of the work was done while the third author was visiting Southwest university in China, which he thanks for the hospitality and financial support. The first and second authors are partially supported financially by NSFC (Nos. 11501468, 11501469). The third author is partially supported by the research fund of Hanyang University (HY-2017).
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Communicated by P. Rabinowitz.
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Chen, W., Deng, S. & Kim, S. Clustered solutions to low-order perturbations of fractional Yamabe equations. Calc. Var. 56, 160 (2017). https://doi.org/10.1007/s00526-017-1253-2
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DOI: https://doi.org/10.1007/s00526-017-1253-2