Long time asymptotic equivalence of the Vlasov-Poisson-Boltzmann equations at the level of the compressible Navier-Stokes-Poisson equations

In this paper, we are concerned with long time asymptotic equivalence between the Vlasov-Poisson-Boltzmann (VPB) system and the compressible Navier-Stokes-Poisson (NSP) system. The density of the VPB system is proved to be asymptotically equivalent (mod decay rate $ (1+t)^{-1} $) as $ t\rightarrow \infty $ to that of the compressible Navier-Stokes-Poisson equations for the corresponding initial data. Regarding the momentum difference, we separately analyze the real and imaginary parts of its Fourier transform. It is shown that the real part decays at a rate of $ (1+t)^{-\frac{3}{4}}\ln(1+t) $, while the imaginary part decays at an optimal rate of $ (1+t)^{-\frac{1}{4}} $.

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Publication Details

Journal
Discrete and Continuous Dynamical Systems
Published
2025-01-01
DOI
https://doi.org/10.3934/dcds.2025050
Primary Topic
Gas Dynamics and Kinetic Theory
Type
article
Field-Weighted Citation Impact
0.00

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article

Long time asymptotic equivalence of the Vlasov-Poisson-Boltzmann equations at the level of the compressible Navier-Stokes-Poisson equations

Yachun Li, Jiahuan Chen
Discrete and Continuous Dynamical Systems
Gas Dynamics and Kinetic Theory
article

Long time asymptotic equivalence of the Vlasov-Poisson-Boltzmann equations at the level of the compressible Navier-Stokes-Poisson equations

Yachun Li, Jiahuan Chen
article en

Abstract

In this paper, we are concerned with long time asymptotic equivalence between the Vlasov-Poisson-Boltzmann (VPB) system and the compressible Navier-Stokes-Poisson (NSP) system. The density of the VPB system is proved to be asymptotically equivalent (mod decay rate $ (1+t)^{-1} $) as $ t\rightarrow \infty $ to that of the compressible Navier-Stokes-Poisson equations for the corresponding initial data. Regarding the momentum difference, we separately analyze the real and imaginary parts of its Fourier transform. It is shown that the real part decays at a rate of $ (1+t)^{-\frac{3}{4}}\ln(1+t) $, while the imaginary part decays at an optimal rate of $ (1+t)^{-\frac{1}{4}} $.

Discrete and Continuous Dynamical SystemsVol. 45(11)
Shanghai Jiao Tong University (CN)
National Natural Science Foundation of China, Fundamental Research Funds for the Central Universities
Openalex Percentile: Top 89%
Gas Dynamics and Kinetic Theory
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