Almost Global Solutions of Kirchhoff Equation
Jianjun Liu, Duohui Xiang
TL;DR
The paper proves almost global existence and stability for the Kirchhoff equation under small initial data by developing a rational normal-form theory for infinite-dimensional reversible vector fields, circumventing the lack of external parameters. It constructs near-identity transformations to iteratively remove non-resonant and non-normal-form interactions, while enforcing a global small-divisor control that is preserved through the iterative steps. The main contributions are explicit long-time stability bounds in Sobolev, Gevrey, and analytic spaces, along with sharp energy-type estimates for the actions, demonstrating sub-exponential time scales in higher-regularity spaces. This approach highlights the distinct behavior of reversible (as opposed to Hamiltonian) vector fields in normal-form analysis and promising avenues toward KAM-type results for Kirchhoff-type systems.
Abstract
This paper is concerned with the original Kirchhoff equation $$\left\{\begin{aligned} & \pa_{tt}u-\Big(1+\int_{0}^π|\pa_xu|^2 dx\Big)\pa_{xx}u=0, \\&u(t,0)=u(t,π)=0. \end{aligned}\right.$$ We obtain almost global existence and stability of solutions for almost any small initial data of size $\varepsilon$. In Sobolev spaces, the time of existence and stability is of order $\varepsilon^{-r}$ for arbitrary positive integer $r$. In Gevrey and analytic spaces, the time is of order $e^{\frac{|\ln\varepsilon|^2}{c\ln|\ln\varepsilon|}}$ with some positive constant $c$. To achieve these, we build rational normal form for infinite dimensional reversible vector fields without external parameters. We emphasize that for vector fields, the homological equation and the definition of rational normal form are significantly different from those for Hamiltonian functions.
