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arXiv 2103.03576math.APmath-phmath.MP
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周期色散Burgers型方程与重力-毛细波方程流映射的正则性结果

Regularity results on the flow maps of periodic dispersive Burgers type equations and the Gravity-Capillary equations

Ayman Rimah Said

AI总结:

本文证明周期色散Burgers方程和重力-毛细波方程的流映射在特定Sobolev空间中的Lipschitz正则性,并验证了先前结果的最优性。

摘要:

本文第一部分证明了具有非局部项$|D|^{\alpha-1} \partial_x u$($\alpha\in[1,+\infty[$)的色散Burgers方程所关联的流,对于$T>0$且$s>\lceil \frac{\alpha}{\alpha-1}\rceil-\frac{1}{2}$,是从$H^s_0(\mathbb{T};\mathbb{R})$的有界集到$C^0([0,T],H^{s-(2-\alpha)^+}_0(\mathbb{T};\mathbb{R}))$的Lipschitz映射,其中$H^s_0$是均值为零的函数的Sobolev空间,从而证明了[37]中在环面上的结果是最优的。证明依赖于T.Tao在[43]中为Benjamin-Ono方程引入的复Cole-Hopf规范变换的仿微分推广。为此,我们证明了双曲仿微分方程流的Baker-Campbell-Hausdorff公式的推广,并证明了在共轭作用下,仿微分算子类在模去更正则的余项后是稳定的。为此,我们证明了Beals[9]精神下仿微分算子的一个新刻画。在本文第二部分,我们使用前述方法的仿微分版本,证明一维周期重力-毛细波方程的流的重整化,对于$T>0$且$s>3+\frac{1}{2}$,是从$H^s$的有界集到$C^0([0,T],H^{s-\frac{1}{2}})$的Lipschitz映射。这证明了[37]中关于水波系统的结果是最优的。

英文摘要:

In the first part of this paper we prove that the flow associated to a dispersive Burgers equation with a non local term of the form $|D|^{α-1} \partial_x u$, $α\in [1,+\infty[$ is Lipschitz from bounded sets of $H^s_0(\mathbb{T};\mathbb{R})$ to $C^0([0,T],H^{s-(2-α)^+}_0(\mathbb{T};\mathbb{R}))$ for $T>0$ and $s>\lceil \fracα{α-1}\rceil-\frac{1}{2}$, where $H^s_0$ are the Sobolev spaces of functions with $0$ mean value, proving that the result obtained in [37] is optimal on the torus. The proof relies on a paradifferential generalization of a complex Cole-Hopf gauge transformation introduced by T.Tao in [43] for the Benjamin-Ono equation. For this we prove a generalization of the Baker-Campbell-Hausdorff formula for flows of hyperbolic paradifferential equations and prove the stability of the class of paradifferential operators modulo more regular remainders, under conjugation by such flows. For this we prove a new characterization of paradifferential operators in the spirit of Beals [9]. In the second part of this paper we use a paradifferential version of the previous method to prove that a re-normalization of the flow of the one dimensional periodic gravity capillary equation is Lipschitz from bounded sets of $H^s$ to $C^0([0,T],H^{s-\frac{1}{2}})$ for $T>0$ and $s>3+\frac{1}{2}$. This proves that the result obtained in [37] is optimal for the water waves system.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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