2018
DOI: 10.1016/s0252-9602(18)30789-6
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Stability of rarefaction wave for a macroscopic model derived from the Vlasov-Maxwell-Boltzmann system

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Cited by 5 publications
(4 citation statements)
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“…Luo-Yao-Zhu in [27] and Yao-Zhu in [40] established the stability of rarefaction wave for the isentropic Navier-Stokes-Maxwell equations and non-isentropic ones under small H 1 -initial perturbations, respectively. What' more, Huang-Liu in [14] consider the stability of rarefaction wave for a macroscopic model derived from the Vlasov-Maxwell-Boltzmann system, in which the model they consider is obviously different from ours in this paper, except for the similar dissipative term E + ub.…”
Section: The Problemmentioning
confidence: 79%
“…Luo-Yao-Zhu in [27] and Yao-Zhu in [40] established the stability of rarefaction wave for the isentropic Navier-Stokes-Maxwell equations and non-isentropic ones under small H 1 -initial perturbations, respectively. What' more, Huang-Liu in [14] consider the stability of rarefaction wave for a macroscopic model derived from the Vlasov-Maxwell-Boltzmann system, in which the model they consider is obviously different from ours in this paper, except for the similar dissipative term E + ub.…”
Section: The Problemmentioning
confidence: 79%
“…established the stability of rarefaction wave for the compressible isentropic and non-isentropic Navier-Stokes-Maxwell equations under suitable smallness conditions, respectively. Huang-Liu in[13] consider the stability of rarefaction wave for a macroscopic model derived from the Vlasov-Maxwell-Boltzmann system, in which the model they consider is obviously different from this in our paper, except for the similar dissipative term E + ub. Recently, Yao-Zhu in[49] study the asymptotic stability of the superposition of viscous contact wave with rarefaction waves for the compressible Navier-Stokes-Maxwell equations, which is the first result on the combination of two different wave patterns of this complex coupled model.…”
mentioning
confidence: 84%
“…Thirdly, in order to absorb some nonlinear bad terms by the single or the compound good term associated with the electromagnetic fields, we require a technical condition (1.29) that dielectric constant ε is bounded for some positive constantsC (depending only on |u ± | and θ − ), see estimates (2.23)-(2.26), (2.31) in Lemma 2.1 and estimates (2.40)-(2.43) in Lemma 2.2. We would like to mention that Huang-Liu in [10] consider the stability of rarefaction wave for a macroscopic model derived from the Vlasov-Maxwell-Boltzmann system. Here we should point out that, except for the similar dissipative term E + ub, the model we consider in this paper is obviously different from that in [10].…”
Section: Huancheng Yao Haiyan Yin and Changjiang Zhumentioning
confidence: 99%
“…We would like to mention that Huang-Liu in [10] consider the stability of rarefaction wave for a macroscopic model derived from the Vlasov-Maxwell-Boltzmann system. Here we should point out that, except for the similar dissipative term E + ub, the model we consider in this paper is obviously different from that in [10]. In contrast to the requirement of smallness of the profile |u r (x, t)| imposed in the proof of [10], in this paper, we require ε•max{|u − | , |u + |} to be small instead, which can not only contain but also extend the condition of [10] in some extent, see Remark 1 for details.…”
Section: Huancheng Yao Haiyan Yin and Changjiang Zhumentioning
confidence: 99%