Reverse Isoperimetric Properties of Thick $λ$-Concave Bodies in the Hyperbolic Plane
Maria Esteban
TL;DR
The paper solves a reverse isoperimetric problem for thick $\lambda$-concave bodies in the hyperbolic plane $\mathbb{H}^2$, identifying the thick $\lambda$-sausage as the unique area minimizer at fixed boundary length under curvature bounds $\tfrac{1}{\lambda} \le \kappa \le \lambda$. The authors develop a hyperbolic Steiner framework and address the non-convexity of inner parallel bodies by leveraging a thickness condition, proving both the minimization result and a sharp lower bound on area that recovers the Euclidean case as curvature tends to zero. A key methodological contribution is a Blaschke-type rolling theorem for thick $\lambda$-concave bodies in $\mathbb{H}^2$, establishing that a ball of curvature $\lambda$ can freely roll inside the body under the thickness assumption, with optimality of this condition. The work bridges Euclidean reverse isoperimetric results with hyperbolic geometry, offering precise characterizations and enabling a robust comparison principle via inner parallel transformations and hyperbolic Steiner-type formulas. These results deepen understanding of convex geometry in spaces of constant negative curvature and have potential implications for geometric optimization under curvature constraints in non-Euclidean settings.
Abstract
In this paper we address the reverse isoperimetric inequality for convex bodies with uniform curvature constraints in the hyperbolic plane $\mathbb{H}^2$. We prove that the\textit{ thick $λ$-sausage} body, that is, the convex domain bounded by two equal circular arcs of curvature $λ$ and two equal arcs of hypercircle of curvature $1 / λ$, is the unique minimizer of area among all bodies $K \subset \mathbb{H}^2$ with a given length and with curvature of $\partial K$ satisfying $1 / λ\leq κ\leq λ$ (in a weak sense). We call this class of bodies \textit{thick $λ$-concave} bodies, in analogy to the Euclidean case where a body is $λ$-concave if $0 \leq κ\leq λ$. The main difficulty in the hyperbolic setting is that the inner parallel bodies of a convex body are not necessarily convex. To overcome this difficulty, we introduce an extra assumption of thickness $κ\geq 1/λ$.
