Geometric interpretation of the vanishing Lie Bracket for two-dimensional rough vector fields
Annalaura Rebucci, Martina Zizza
TL;DR
The paper addresses the problem of when the commutativity of flows generated by two vector fields $X$ and $Y$ is equivalent to the vanishing Lie bracket $[X,Y]$ in rough, two-dimensional settings. It develops a geometric, Hamiltonian-based approach that, in 2D, shows $[X,Y]=0$ implies $ ext{flow}_t^X ext{flow}_s^Y= ext{flow}_s^Y ext{flow}_t^X$ for continuous $X,Y$ with bounded divergence, removing the need for weak Lie differentiability. The authors first treat the Hamiltonian divergence-free case, exploiting level-set structure and the identity $X eq 0$ and $X= abla^ot H$, $Y= abla^ot K$, with $[X,Y]=0$ equivalent to $X\,\cdot\,Y^\perp=\text{const}$, and then extend to nearly incompressible fields via invariant regions $\,\Omega_\kappa$ and a density-based reparameterization. They also discuss a BV extension and outline open questions for the reverse implication in the BV setting. Overall, the work advances Frobenius-type results for flows of rough vector fields in the plane and highlights geometric structures that govern commutativity in low dimensions with potential PDE applications.
Abstract
In this paper, we prove that if $X,Y$ are continuous, Sobolev vector fields with bounded divergence on the real plane and $[X,Y]=0$, then their flows commute. In particular, we improve the previous result of Colombo-Tione (2021), where the authors require the additional assumption of the weak Lie differentiability on one of the two flows. We also discuss possible extensions to the $\text{BV}$ setting.
