Upper bound for the total mean curvature of spin fill-ins
Christian Baer
TL;DR
This work proves Gromov's conjecture on an upper bound for the total mean curvature of the boundary of a spin fill-in under a scalar curvature lower bound, in the case that the boundary mean curvature is nonnegative. The authors derive a dimension-dependent inequality $\int_M H \le C(M) + \sqrt{\frac{n}{n+1}}\,\lambda\,\mathrm{vol}(M)$ for spin fill-ins with $\mathrm{scal}_X \ge -\lambda^2$, where $C(M)$ depends only on the boundary manifold's spin structure. The proof deploys boundary value problems for the Dirac operator, a carefully constructed boundary constant $C(M)$ built from intrinsic Dirac data on $M$, and a Weitzenböck-type estimate with a modified connection to control boundary terms. The results connect scalar curvature, mean curvature, and spin geometry to provide a quantitative, geometry-driven bound with explicit dependence on $\lambda$ and the boundary volume, matching known sharp cases in special geometries.
Abstract
Gromov conjectured that the total mean curvature of the boundary of a compact Riemannian manifold can be estimated from above by a constant depending only on the boundary metric and on a lower bound for the scalar curvature of the fill-in. We prove Gromov's conjecture if the manifolds are spin and the mean curvature is non-negative.
