Mean curvature bounds and eigenvalues of Robin Laplacians

preprint2014arXivOpen access

Abstract

We consider the Laplacian with attractive Robin boundary conditions, QαΩu=−Δu,∂u∂n=αu on ∂Ω, Q^Ω_αu=-Δu, \quad \dfrac{\partial u}{\partial n}=αu \text{ on } \partialΩ, in a class of bounded smooth domains Ω∈RνΩ\in\mathbb{R}^ν; here nn is the outward unit normal and α>0α>0 is a constant. We show that for each j∈Nj\in\mathbb{N} and α→+∞α\to+\infty, the jjth eigenvalue Ej(QαΩ)E_j(Q^Ω_α) has the asymptotics Ej(QαΩ)=−α2−(ν−1)Hmax(Ω) α+O(α2/3), E_j(Q^Ω_α)=-α^2 -(ν-1)H_\mathrm{max}(Ω)\,α+{\mathcal O}(α^{2/3}), where Hmax(Ω)H_\mathrm{max}(Ω) is the maximum mean curvature at ∂Ω\partial Ω. The discussion of the reverse Faber-Krahn inequality gives rise to a new geometric problem concerning the minimization of HmaxH_\mathrm{max}. In particular, we show that the ball is the strict minimizer of HmaxH_\mathrm{max} among the smooth star-shaped domains of a given volume, which leads to the following result: if BB is a ball and ΩΩ is any other star-shaped smooth domain of the same volume, then for any fixed j∈Nj\in\mathbb{N} we have Ej(QαB)>Ej(QαΩ)E_j(Q^B_α)>E_j(Q^Ω_α) for large αα. An open question concerning a larger class of domains is formulated.

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