Extending the flux homomorphism to volume-preserving homeomorphisms
Stéphane Tchuiaga
TL;DR
The work develops a $C^0$-robust extension of the flux homomorphism to volume-preserving homeomorphisms by introducing gap functions $\mathbf{R}_\delta(H,\alpha)$ and an extended flux $\widetilde{L}_\Omega^\delta$, establishing a precise factorization with the smooth flux and a Poincaré-duality framework via Fathi’s mass flow. A central result is the $(C^0,\delta)$-rigidity: the extended flux group $\tilde{\Gamma}_\Omega^\delta$ coincides with the classical flux group $\Gamma_\Omega$, indicating that small $C^0$ perturbations do not enlarge the flux possibilities. The paper also develops a cohomological perspective for $Homeo_0(M,\Omega)$, showing a natural injection of $H^1(M,\mathbb{R})$ into $H^1(Homeo_0(M,\Omega),\mathcal{C}(M,\mathbb{R}))$ and a lower bound on the first cohomology, thereby linking topology to dynamical constraints. Collectively, these results bridge smooth and topological dynamics for volume-preserving maps, propose a norm measuring form-distortion under homeomorphisms, and lay groundwork for rigidity phenomena and energy considerations in symplectic topology and related conservative systems.
Abstract
This paper extends the flux homomorphism to volume-preserving homeomorphisms. A surprising $(C^0, δ)-$rigidity result where the extended flux groups coincide with the standard flux group is proved. The introduced tools, which also include a Poincaré duality with Fathi's mass flow and a norm on the group of volume-preserving homeomorphisms, indicate a potential for new flexibility in the behavior of homeomorphisms. This flexibility could have implications for rigidity results in symplectic/cosymplectic geometry, particularly those concerning Lefschetz manifolds: Any finite energy symplectic homeomorphism of $(T^2, ω)$ with trivial flux, is a finite energy Hamiltonian homeomorphism of $(T^2, ω)$. We discuss the cohomology groups $H^\ast(Homeo_0(M,Ω), \mathcal{C}(M, \mathbb{R}) )$ of $ Homeo_0(M,Ω)$ with coefficients in $ \mathcal{C}(M, \mathbb{R})$.
