Table of Contents
Fetching ...

Long time dynamics of space periodic water waves

Massimiliano Berti

TL;DR

The work surveys long-time dynamics of space-periodic water waves, focusing on three pillars: the emergence of quasi-periodic solutions via KAM for 1d quasi-linear PDEs, long-time well-posedness through paradifferential Birkhoff normal form, and rigorous modulational instability analyses of Stokes waves. It introduces and integrates novel techniques—pseudo-differential KAM, paradifferential BNF, and symplectic Kato perturbation—to handle the quasi-linear, nonlocal Dirichlet–Neumann structure and reversible Hamiltonian nature of the water-wave equations. Key results include the existence of small-amplitude quasi-periodic standing and traveling waves, almost global-in-time stability for small data, and precise descriptions of modulational instabilities near Stokes waves (figure-8 near zero and high-frequency isolas). Collectively, these contributions illuminate how Hamiltonian structure and spectral methods govern the long-time dynamics of space-periodic water waves and point to important open problems in higher dimensions and broader parameter regimes.

Abstract

We review recent advances regarding the long-time dynamics of space-periodic water waves, focusing on 1) bifurcation of quasi-periodic solutions, both standing and traveling; 2) long-time well-posedness results; 3) modulational instability of Stokes waves. These results rely on unconventional approaches to KAM and Birkhoff normal form theories for Hamiltonian quasi-linear PDEs and symplectic Kato perturbation theory for separated eigenvalues of reversible and Hamiltonian operators.

Long time dynamics of space periodic water waves

TL;DR

The work surveys long-time dynamics of space-periodic water waves, focusing on three pillars: the emergence of quasi-periodic solutions via KAM for 1d quasi-linear PDEs, long-time well-posedness through paradifferential Birkhoff normal form, and rigorous modulational instability analyses of Stokes waves. It introduces and integrates novel techniques—pseudo-differential KAM, paradifferential BNF, and symplectic Kato perturbation—to handle the quasi-linear, nonlocal Dirichlet–Neumann structure and reversible Hamiltonian nature of the water-wave equations. Key results include the existence of small-amplitude quasi-periodic standing and traveling waves, almost global-in-time stability for small data, and precise descriptions of modulational instabilities near Stokes waves (figure-8 near zero and high-frequency isolas). Collectively, these contributions illuminate how Hamiltonian structure and spectral methods govern the long-time dynamics of space-periodic water waves and point to important open problems in higher dimensions and broader parameter regimes.

Abstract

We review recent advances regarding the long-time dynamics of space-periodic water waves, focusing on 1) bifurcation of quasi-periodic solutions, both standing and traveling; 2) long-time well-posedness results; 3) modulational instability of Stokes waves. These results rely on unconventional approaches to KAM and Birkhoff normal form theories for Hamiltonian quasi-linear PDEs and symplectic Kato perturbation theory for separated eigenvalues of reversible and Hamiltonian operators.
Paper Structure (16 sections, 5 theorems, 49 equations, 3 figures)

This paper contains 16 sections, 5 theorems, 49 equations, 3 figures.

Key Result

Theorem 1.1

(Quasi-periodic standing water waves BBHM) Consider finitely many "tangential" sites $\mathbb{S}^+ \subset \mathbb N$ and denote $\nu := | \mathbb{S}^+|$ its cardinality. Fix a subset $[\mathtt{h}_1, \mathtt{h}_2 ] \subset (0,+\infty)$. Then there exists $\bar{s} > 0$, $\varepsilon_0 \in (0,1)$ such In addition the quasi-periodic solutions QP:soluz0 are linearly stable.

Figures (3)

  • Figure 1: The gravity water waves problem. The velocity field inside the time dependent domain $\mathcal{D}_\eta$ is divergence free and with constant vorticity $\gamma$. Capillary forces may act at the free interface $y = \eta (t,x)$.
  • Figure 2: On the left, standing waves for irrotational fluids ($\gamma =0$); these solutions are even in $x$ at any time. On the right, quasi-periodic traveling Stokes waves with $\nu$ frequencies, see \ref{['def:QPT']}.
  • Figure 3.1: spectral bands with non zero real part of the $L^2 (\mathbb R)$-spectrum of $\mathcal{L}_{\varepsilon}$. The "figure 8" is present for $\mathtt{h} > 1.363...$. For any ${\mathtt p} \geq 2$, for any depth except a closed set, there exists an isola of instability with size $\propto | \beta_1^{(\mathtt{p})}(\mathtt{h})| \varepsilon^{{\mathtt p} }$. Its center $y_0^{({\mathtt p} )} (\varepsilon)$ is $\mathcal{O}(\varepsilon^2)$ distant from ${\rm i} \omega_*^{({\mathtt p} )}$. The notation $a \propto b$ means that $a b^{-1} \to c$ as $\varepsilon \to 0$.

Theorems & Definitions (7)

  • Theorem 1.1
  • Definition 1.2
  • Theorem 1.3
  • Theorem 2.1
  • Remark 3.1
  • Theorem 3.2
  • Theorem 3.3: High frequency instabilities BCMV