Linear Landau Damping for the Vlasov-Maxwell System in \(\mathbb{R}^3\)

IF 2.6 1区 数学 Q1 MATHEMATICS
Daniel Han-Kwan, Toan T. Nguyen, Frédéric Rousset
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引用次数: 0

Abstract

In this work, we consider the relativistic Vlasov-Maxwell system, linearized around a spatially homogeneous equilibrium, set in the whole space \(\mathbb{R}^3 \times \mathbb{R}^3\). The equilibrium is assumed to belong to a class of radial, smooth, rapidly decaying functions. Under appropriate conditions on the initial data, we prove algebraic decay (of dispersive nature) for the electromagnetic field. For the electric scalar potential, the leading behavior is driven by a dispersive wave packet with non-degenerate phase and compactly supported amplitude, while for the magnetic vector potential, it is driven by a wave packet whose phase behaves globally like the one of Klein-Gordon and the amplitude has unbounded support.

Vlasov-Maxwell系统的线性朗道阻尼 \(\mathbb{R}^3\)
在这项工作中,我们考虑了相对论性的Vlasov-Maxwell系统,它围绕一个空间均匀平衡线性化,设置在整个空间\(\mathbb{R}^3 \times \mathbb{R}^3\)。该平衡被假定为一类径向、光滑、快速衰减的函数。在初始数据的适当条件下,我们证明了电磁场的代数衰减(色散性质)。对于标量势,主导行为是由相位非简并且幅值紧支持的色散波包驱动的,而对于矢量势,主导行为是由相位像Klein-Gordon一样具有全局行为且幅值具有无界支持的波包驱动的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Annals of Pde
Annals of Pde Mathematics-Geometry and Topology
CiteScore
3.70
自引率
3.60%
发文量
22
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