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Critical Robin Problems on Manifolds with Noncompact Boundary

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Abstract · v1

We work on connected, noncompact nn-dimensional Riemannian manifolds (M,g),n≥3(\mathcal{M}, g), n \geq 3, that are complete with respect to dgd_g and have noncompact boundary and bounded geometry. We study the existence of positive solutions in C∞(M)∩L2∗(M)∩L∞(M)C^{\infty}(\mathcal{M}) \cap L^{2^*}(\mathcal{M}) \cap L^{\infty}(\mathcal{M}) to the Yamabe problem: {−Δgu+n−24(n−1)Rgu=C0un+2n−2 in M,∂u∂ν+n−22(n−1)Hgu=C1unn−2 on ∂M, \left\{\begin{aligned} -Δ_g u+\frac{n-2}{4(n-1)} R_g u & =\mathscr{C}_0 u^{\frac{n+2}{n-2}} \quad \text { in } \mathcal{M}, \\ \frac{\partial u}{\partial ν}+\frac{n-2}{2(n-1)} H_g u & =\mathscr{C}_1 u^{\frac{n}{n-2}} \quad \text { on } \partial \mathcal{M}, \end{aligned}\right. where C0=YC(M),C1=YC(M)Cdˉ2n−2\mathscr{C}_0=Y_{\mathscr{C}}(\mathcal{M}), \mathscr{C}_1=Y_{\mathscr{C}}(\mathcal{M}) \mathscr{C} \bar{d}^{\frac{2}{n-2}}, the parameter C≥0\mathscr{C} \geq 0 is fixed, and YC(M):=inf⁡u∈Cc∞(M)\{0}Eg(u)(∥u∥L2∗(M)2∗+C∥u∥L2#(∂M)2∗)2/2∗. Y_{\mathscr{C}}(\mathcal{M}):=\inf _{u \in C_c^{\infty}(\mathcal{M}) \backslash\{0\}} \frac{E_g(u)}{\left(\|u\|_{L^{2^*}(\mathcal{M})}^{2^*}+\mathscr{C}\|u\|_{L^{2^{\#}}(\partial \mathcal{M})}^{2^*}\right)^{2 / 2^*}} . Here EgE_g is the associated quadratic energy. We assume YC(M)<YC,∞(M)Y_{\mathscr{C}}(\mathcal{M})<Y_{\mathscr{C}, \infty}(\mathcal{M}) and YC,∞(M)>0Y_{\mathscr{C}, \infty}(\mathcal{M})>0, where YC,∞Y_{\mathscr{C}, \infty} is the corresponding variational level at infinity. We approach this problem using nonnegative solutions uj∈W∂1,2(Bg(O,j)),j∈N,j≥j0u_j \in W_{\partial}^{1,2}\left(B_g(\mathcal{O}, j)\right), j \in \mathbb{N}, j \geq j_0, for which we prove that sup⁡j≥j0∥uj∥L∞(Bg(O,j−1))<∞. \sup _{j \geq j_0}\left\|u_j\right\|_{L^{\infty}\left(B_g(\mathcal{O}, j-1)\right)}<\infty . For C>0\mathscr{C}>0, we also prove that, along a subsequence, ∥uj∥L2(Bg(O,j)∩∂M)→dˉ\left\|u_j\right\|_{L^2{ }_{\left(B_g(\mathcal{O}, j) \cap \partial \mathcal{M}\right)}} \rightarrow \bar{d}, with 0<dˉ≤C−1/2∗0<\bar{d} \leq \mathscr{C}^{-1 / 2^*}. For C=0\mathscr{C}=0, we set dˉ=0\bar{d}=0.

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