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Turbulence in Magnetized Pair Plasmas

机译:磁化对等离子体中的湍流

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Alfvénic-type turbulence in strongly magnetized, low-beta pair plasmas is investigated. A coupled set of equations for the evolution of the magnetic and flow potentials are derived, covering both fluid and kinetic scales. In the fluid (magnetohydrodynamic) range those equations are the same as for electron-ion plasmas, so turbulence at those scales is expected to be of the Alfvénic nature, exhibiting critical balance, dynamic alignment, and transition to a tearing-mediated regime at small scales. The critical scale at which a transition to a tearing-mediated range occurs is derived, and the spectral slope in that range is predicted to be k~(-8/3)_⊥ (or k~(-3)_⊥, depending on details of the reconnecting configuration assumed). At scales below the electron (and positron) skin depth, it is argued that turbulence is dictated by a cascade of the inertial Alfvén wave, which we show to result in the magnetic energy spectrum ∝ k~(-11/3)_⊥.
机译:研究了强烈磁化,低β对等离子体的Alfvénic型湍流。 推导出用于磁性和流动电位的演化的耦合方程组,覆盖流体和动力学尺度。 在流体(磁流动动力学)范围内,那些方程式与电子离子等离子体相同,因此这些尺度的湍流预计将成为阿法尼性质,表现出临界平衡,动态对准,并在小的撕裂介导的方案过渡 秤。 推导出过渡到撕裂介导范围的临界量表,并且该范围内的光谱斜率预测为k〜(-8/3)_⊥(或k〜(-3)_⊥,取决于 关于假设重新连接配置的细节)。 在电子(和正电子和正电子)下方的刻度下,认为湍流由惯性Alfvén波的级联决定,我们展示导致磁能谱αk〜(-11/3)_⊥。

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