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Nonlinear saturation of the Weibel instability in a dense Fermi plasma

机译:密费米等离子体中Weibel不稳定性的非线性饱和

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We present an investigation for the generation of intense magnetic field in dense plasmas with an anisotropic electron Fermi-Dirac distribution. For this purpose, we use a new linear dispersion relation for transverse waves in the Wigner Maxwell dense quantum plasma system. Numerical analysis of the dispersion relation reveals the scaling of the growth rate as a function of the Fermi energy and the temperature anisotropy. The nonlinear saturation level of the magnetic fields is found through fully kinetic simulations. which indicates that the final amplitudes of the magnetic fields are proportional to the linear growth rate of the instability. The present results are important for understanding the origin of intense magnetic fields in dense Fermionic plasmas, such as those in the next-generation intense laser solid density plasma experiments.
机译:我们提出了在各向异性电子费米-狄拉克分布的稠密等离子体中产生强磁场的研究。为此,我们在Wigner Maxwell密集量子等离子体系统中对横向波使用了新的线性色散关系。色散关系的数值分析表明,增长率是费米能量和温度各向异性的函数。磁场的非线性饱和度是通过完全动力学模拟得出的。这表明磁场的最终振幅与不稳定性的线性增长率成正比。目前的结果对于理解密集的费米离子等离子体中的强磁场起源很重要,例如下一代强激光固体密度等离子体实验中的强磁场。

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