A functional characterization of isometries between non-reversible Finsler manifolds
Francisco Venegas M
TL;DR
The paper addresses the problem of functionally characterizing isometries between non-reversible Finsler manifolds. It introduces an asymmetric function-space framework, constructing the extended asymmetric normed algebra $oxed{\mathcal{A}(\mathcal{X})}$ from the cone of smooth semi-Lipschitz functions, and proves a non-reversible Myers-Nakai-type theorem: an isomorphism of these algebras yields a Finsler isometry with explicit bi-semi-Lipschitz control. This establishes a Banach-Stone-type correspondence in fully asymmetric Finsler geometry and extends prior reversible/quasi-reversible results by leveraging quasi-metric and conic-algebraic structures. The work provides a robust functional-analytic mechanism to recover geometric isometries in non-symmetric settings, with potential implications for understanding the interplay between quasi-metric spaces and differential-geometric structures.
Abstract
We provide a functional characterization of isometries between non-reversible Finsler manifolds, in the form of a generalization of the Myers-Nakai Theorem for Riemannian manifolds. We show that, since non-reversible Finsler manifolds are a fundamentally asymmetric object, such a result can not be obtained by means of a symmetric function space, and we define the appropriate asymmetric structure needed to describe all possible isometries between this class of manifolds. The result is based on the ideas used in a previous generalization for reversible Finsler manifolds proved in \cite{GJR-13}, in which the normed algebra of $C^1$-smooth Lipschitz functions is used. To reflect the quasi-metric structure of non-reversible Finsler manifolds, this normed algebra had to be modified to include the cone of smooth semi-Lipschitz functions, resulting in a partial loss of the normed space and algebra structures. In order to achieve the desired result, we define new algebraic/quasi-metric structures to model the behavior of the aforementioned function space.
