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非广延电子-正电子等离子体中的朗缪尔振荡

Langmuir oscillations in a nonextensive electron-positron plasma.

作者信息

Saberian E, Esfandyari-Kalejahi A

机构信息

Department of Physics, Faculty of Sciences, Azarbaijan Shahid Madani University, P. O. Box 53714-161, 5375171379 Tabriz, Iran.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2013 May;87(5):053112. doi: 10.1103/PhysRevE.87.053112. Epub 2013 May 30.

DOI:10.1103/PhysRevE.87.053112
PMID:23767648
Abstract

The Langmuir oscillations, Landau damping, and growing unstable modes in an electron-positron (EP) plasma are studied by using the Vlasov and Poisson's equations in the context of the Tsallis's nonextensive statistics. Logically, the properties of the Langmuir oscillations in a nonextensive EP plasma are remarkably modified in comparison with that of discussed in the Boltzmann-Gibbs statistics, i.e., the Maxwellian plasmas, because of the system under consideration is essentially a plasma system in a nonequilibrium stationary state with inhomogeneous temperature. It is found that by decreasing the nonextensivity index q which corresponds to a plasma with excess superthermal particles, the phase velocity of the Langmuir waves increases. In particular, depend on the degree of nonextensivity, both of damped and growing oscillations are predicted in a collisionless EP plasma, arise from a resonance phenomena between the wave and the nonthermal particles of the system. Here, the mechanism leads to the unstable modes is established in the context of the nonextensive formalism yet the damping mechanism is the same developed by Landau. Furthermore, our results have the flexibility to reduce to the solutions of an equilibrium Maxwellian EP plasma (extensive limit q→1), in which the Langmuir waves are only the Landau damped modes.

摘要

在Tsallis非广延统计框架下,通过使用Vlasov方程和泊松方程研究了电子 - 正电子(EP)等离子体中的朗缪尔振荡、朗道阻尼和增长的不稳定模式。从逻辑上讲,与玻尔兹曼 - 吉布斯统计(即麦克斯韦等离子体)中讨论的情况相比,非广延EP等离子体中朗缪尔振荡的特性有显著改变,这是因为所考虑的系统本质上是一个处于非平衡稳态且温度不均匀的等离子体系统。研究发现,通过降低对应于具有过量超热粒子等离子体的非广延性指数q,朗缪尔波的相速度会增加。特别地,取决于非广延程度,在无碰撞EP等离子体中预测了阻尼振荡和增长振荡,这是由波与系统中的非热粒子之间的共振现象引起的。在此,导致不稳定模式的机制是在非广延形式体系的背景下建立的,而阻尼机制与朗道所发展的相同。此外,我们的结果可以灵活地简化为平衡麦克斯韦EP等离子体(广延极限q→1)的解,其中朗缪尔波仅是朗道阻尼模式。

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