On the Gevrey regularity of the fifth-order Kadomtsev-Petviashvili-II equation: An improved approach
Aissa Boukarou, Lamia Seghour
TL;DR
This work establishes sharp temporal Gevrey regularity for the 2+1D fifth-order KP-II equation: if the initial data are Gevrey of order $\sigma$ in space, the solution is Gevrey of order $5\sigma$ in time, and it cannot belong to $G^z$ for any $1 \le z < 5\sigma$. The authors introduce a refined majorant-series method in Gevrey–Bourgain spaces to track the dispersive term $\partial_x^5u$ and nonlinear interactions, and they prove a general principle for dispersive equations of the form $\partial_t u = \pm \partial_x^\alpha u + P(u)$ that temporal Gevrey regularity below $\alpha\sigma$ cannot hold. A key part of the argument is constructing data that forces growth like $((5j)!)^\sigma$ in time derivatives, establishing the optimality of the $5\sigma$ rate. The results extend prior work by Boukarou et al. and provide a robust analytic framework for temporal Gevrey regularity in higher-order dispersive PDEs, with the Kawahara equation discussed as a canonical example.
Abstract
In this paper, we improve and extend the results obtained by Boukarou et al. \cite{boukarou1} on the Gevrey regularity of solutions to a fifth-order Kadomtsev-Petviashvili-II equation. We establish Gevrey regularity in the time variable for solutions in $2+1$ dimensions, providing a sharper result obtained through a new analytical approach. Assuming that the initial data are Gevrey regular of order $σ\geq 1$ in the spatial variables, we prove that the corresponding solution is Gevrey regular of order $5 σ$ in time. Moreover, we show that the function $u(x, y, t)$, viewed as a function of $t$, does not belong to $G^z$ for any $1 \leq z<5 σ$. Our proof introduces a new analytical method that establishes a general principle for dispersive equations of the form $ \partial_t u = \pm\partial_x^αu + P(u),$ where $\partial_x^α$ is the highest spatial derivative and $P(u)$ a polynomial in spatial derivatives of total order at most $α-1$, the solution cannot belong to the Gevrey class $G^z$ in time for any $z$ satisfying $1 \leq z<ασ$.
