Rigidity of a class of smooth singular flows on $\mathbb T^2$

TL;DR

This paper investigates the rigidity properties of certain smooth singular flows on the 2-torus, establishing conditions for flow disjointness and demonstrating joining rigidity for a broad class of these flows with specific frequency parameters.

Contribution

It introduces a new class of smooth singular flows on the 2-torus and proves joining rigidity results, addressing a problem posed by Ratner.

Findings

Flow disjointness determined by integrals of associated 1-forms.

Existence of a unique frequency for each flow in the class.

Full measure set of frequencies yields joining rigidity for smooth time changes.

Abstract

We study joining rigidity in the class of von Neumann flows with one singularity. They are given by a smooth vector field $\mathcal{X}$ on $\mathbb T^2\setminus \{a\}$, where $\mathcal{X}$ is not defined at $a\in \mathbb T^2$. It follows that the phase space can be decomposed into a (topological disc) $D_\mathcal{X}$ and an ergodic component $E_\mathcal{X}=\mathbb T^2\setminus D_\mathcal{X}$. Let $\omega_\mathcal{X}$ be the 1-form associated to $\mathcal{X}$. We show that if $|\int_{E_{\mathcal{X}_1}}d\omega_{\mathcal{X}_1}|\neq |\int_{E_{\mathcal{X}_2}}d\omega_{\mathcal{X}_2}|$, then the corresponding flows $(v_t^{\mathcal{X}_1})$ and $(v_t^{\mathcal{X}_2})$ are disjoint. It also follows that for every $\mathcal{X}$ there is a uniquely associated frequency $\alpha=\alpha_{\mathcal{X}}\in \mathbb T$. We show that for a full measure set of $\alpha\in \mathbb T$ the class of smooth time changes of $(v_t^\mathcal{X_\alpha})$ is joining rigid, i.e. every two smooth time changes are either cohomologous or disjoint. This gives a natural class of flows for which the answer to a problem of Ratner (Problem 3 in \cite{Rat4}) is positive.