The Funk-Finsler Structure in the Constant Curvature Spaces
Ashok Kumar, Hemangi Madhusudan Shah, Bankteshwar Tiwari
TL;DR
This work identifies and analyzes the infinitesimal Funk-Finsler structure in spaces of constant curvature, presenting a Randers representation $\mathcal{F}_{\epsilon}=\alpha+\beta$ with explicit $\alpha$ and closed $\beta$ for $\epsilon\in\{−1,0,1\}$. It computes the spray coefficients, $S$-curvature, Riemann curvature, Ricci curvature, and flag curvature, proving projective flatness and establishing sharp curvature bounds: $S$-curvature bounds depend on $\epsilon$ (equality only in the Euclidean case) and flag curvature bounds satisfy $K\le -\tfrac{1}{4}$ (hyperbolic), $K\ge -\tfrac{1}{4}$ (spherical), and $K\equiv -\tfrac{1}{4}$ (Euclidean). The paper also provides a Zermelo navigation description of the Funk-Finsler metric on the disc and includes an appendix with the spherical distance formulas essential to the spherical case. Together, these results advance Hilbert-like investigations in constant-curvature Finsler geometries by making the infinitesimal structure explicit and computable.
Abstract
In this paper, we {\it find} the infinitesimal structure of Funk-Finsler metric in spaces of constant curvature. We investigate the geometry of this Funk-Finsler metric by explicitly computing its $S$-curvature, Riemann curvature, Ricci curvature, and flag curvature. Moreover, we show that the $S$-curvature of the Funk-Finsler metric in hyperbolic space is bounded above by $\frac{3}{2}$, in spherical space bounded below by $\frac{3}{2}$, and in Euclidean case it is identically equal to $\frac{3}{2}$. Further, we show that the flag curvature of the Funk-Finsler metric in hyperbolic space is bounded above by $-\frac{1}{4}$, in spherical space bounded below by $-\frac{1}{4}$, and in Euclidean case it is identically equal to $-\frac{1}{4}$.
