Combinatorial structures of the space of Hamiltonian vector fields on compact surfaces

Tomoo Yokoyama

Home/Archive/arXiv

arXiv · 2112.03475

Combinatorial structures of the space of Hamiltonian vector fields on compact surfaces

Tomoo Yokoyama

View original source ↗Read source document ↗Export metadata ↓

Abstract

In the time evolution of fluids, the topologies of fluids can be changed by the creations and annihilations of singular points and by switching combinatorial structures of separatrices. In this paper, to describe the possible generic time evolution of Hamiltonian vector fields on surfaces with or without constraints, we study the structure of the ``moduli space'' of such vector fields under the non-existence of creations and annihilations of singular points. In fact, we describe the relations of bifurcations between Hamiltonian vector fields to construct foundations of descriptions of the time evaluations of fluid phenomena. Moreover, we show that the space of topologically equivalence classes of such vector fields has non-contractible connected components and is a disjoint union of finite abstract cell complexes such that the codimension of a cell corresponds to the instability of a Hamiltonian vector field by using combinatorics and simple homotopy theory. In particular, there is a connected component of the space that is weakly homotopic to a three-dimensional sphere.

Explore related subjects

math.DS

Keep this discovery

BibTeX RIS

Tomoo Yokoyama. 2021-12-07. Combinatorial structures of the space of Hamiltonian vector fields on compact surfaces. https://arxiv.org/abs/2112.03475

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

arXiv2026

Admissible Fourier Lengths, KAM Reducibility, and Spectral Applications

We develop a perturbative KAM reducibility theory for one-frequency $\mathrm{SL}(2,\mathbb{R})$ cocycles based on an admissible Fourier length $\ell$. The regularity relevant to the iteration is measured by positive adapted Fourier width rather than ordinary smoothness in the Euclidean length $|n|$. The same length governs Fourier decay, truncation and resonance scales, and the arithmetic condition controlling the small divisors. This framework contains the classical analytic and Gevrey settings, while non-monotone choices of $\ell$ allow classical nowhere differentiable Weierstrass-type perturbations and continuous perturbations outside every positive H\"older class. As spectral applications, we obtain purely absolutely continuous spectrum for every phase and $1/2$-H\"older continuity of the integrated density of states for the associated quasiperiodic Schr\"odinger operators. The Aubry dual has pure point spectrum for Lebesgue almost every dual phase, with eigenfunctions exponentially localized in the metric induced by $\ell$. We also construct nowhere differentiable quasiperiodic potentials with purely absolutely continuous Cantor spectrum.

math.DS↗

arXiv2026

Dynamics inside the attracting basins of some skew products

Polynomial skew products in $\mathbb{C}^2$ are maps of the form $F(z,w)=(P(z),Q(z,w))$, where $P$ and $Q$ are polynomials. Their local dynamics have been widely investigated. In this paper, we study the global dynamics inside Fatou components of some skew products. We consider all the inverse images in a Fatou component of a given point and use the Kobayashi metric to measure the distance between points. In the cases we consider, there are always arbitrarily large Kobayashi balls in the complement of these inverse sets.

math.DS↗

arXiv2026

Ergodicity of dynamical systems without uniqueness of orbits

Recently, there has been considerable interest in the study of non-deterministic dynamical systems. To analyze the chaotic behavior of such systems from a measure-theoretic viewpoint, it is desirable to consider ergodicity. However, the classical definition of ergodicity involves invariant sets, whose definition is not unique for non-deterministic dynamical systems. Thus, we are led to the question of which invariance yields an interesting definition of ergodicity. Here, we propose a definition based on the strong backward invariance and show that analogs of classical results hold. We also consider implications of the Birkhoff ergodic theorem for systems without uniqueness of orbits.

math.DS↗