Sharp thresholds for the Escobar functional: the Escobar-Willmore mass, geometric selection, and compactness trichotomy

Abstract

We study the hemisphere threshold for the conformally covariant Escobar functional on compact Riemannian manifolds (Mn,g) with boundary. The near-threshold landscape is organized by boundary invariants: the first-order coefficient ρnconfHg vanishes identically, so the leading obstruction is a renormalized boundary mass Rg (second order, n5), followed by a cubic invariant Θg (third order, n6), with a Green kernel interaction G∂ in the multi-bubble regime. Exact evaluation of weighted profile moments yields κ1=κ2=0: the coefficients of Ricg(ν,ν) and Scal g in the bare mass vanish. On \Hg=0\ the mass reduces to Rgbare=6-n2(n-1)(n-3)(n-4)|II|2. The Lyapunov--Schmidt correction gives Rgred Rgbare0 for n6; for n=5 the nonlocal back-reaction overcomes the positive bare coefficient. In every dimension n5, non-umbilic boundaries are automatically subcritical: C*Esc<S whenever II≠0. At threshold, on manifolds not conformally diffeomorphic to the hemisphere, every blow-up of positive constrained critical points is one-bubble and concentrates at an umbilic point with Rg=0, ∇∂ Rg=0. Since Rgred<0 at every non-umbilic point, threshold concentration occurs only on the umbilic stratum \II=0\. There Θg governs the next bifurcation: Θg<0 forces subcriticality; for n7, Θg>0 yields compactness and hemispherical rigidity. In the multi-bubble regime we establish global compactness at Escobar multiples with equal-mass quantization and conditional exclusion of pure multi-bubbling.

0

Turn this paper into a full lesson

ArcXiv compiles a staged curriculum from this paper: 8-12 lessons across beginner → advanced, synthesised section guides, visuals, flashcards, a quiz, exercises, and on-demand deep dives per section. Grounded in the abstract, never invented.

Discussion (0)

Sign in to join the discussion.

Loading comments…