Extremal-parameter conjecture for the biharmonic problem PλP_{\lambda}

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Let n>4n>4, let B1B_1 be the unit ball, and consider the boundary-value problem

{Δ2u=λun+4n−4in B1,u=1on ∂B1,∂u∂n=−n−42on ∂B1.\begin{cases} \Delta^{2}u=\lambda u^{\frac{n+4}{n-4}} & \text{in } B_{1},\\ u=1 & \text{on } \partial B_{1},\\ \frac{\partial u}{\partial n}=-\frac{n-4}{2} & \text{on } \partial B_{1}. \end{cases}

Extremal-parameter conjecture. The extreme value for PλP_{\lambda} is

λ∗=n3(n−4)16.\lambda^{*}=\frac{n^{3}(n-4)}{16}.

The preceding analysis gives at most two solutions for 0<λ<n3(n−4)160<\lambda<\frac{n^{3}(n-4)}{16}, a unique solution at the proposed extremal value, and no solution above it. If the conjecture holds, it yields a hemisphere rigidity theorem under the stated lower bound on the QQ-curvature, boundary agreement with the standard metric, and totally geodesic boundary; a geometric explanation for the extremal curvature bound remains open.

References

Primary source

Mijia Lai and Wei Wei, “Gelfand problem and Hemisphere rigidity”, arXiv:2102.10360 (2022).

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