磁化冷等离子体的拓扑相、拓扑相变和体边对应

Yichen Fu, H. Qin
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引用次数: 1

摘要

等离子体作为拓扑材料近年来得到了广泛的研究。我们试图对磁化冷等离子体的拓扑相、拓扑相变和体边对应有一个全面的了解。我们发现在密度$n$,磁场$B$,并行波数$k_{\parallel}$的参数空间中存在10个拓扑相。它们被朗缪尔波- l波共振、朗缪尔波-回旋波共振和零磁场表面分开。对于固定的$B$和$k_{\parallel}$,只有Langmuir波-回旋波共振的相变对应于边缘模式。给出了这种新型边缘模态存在的充分必要条件,并用数值解进行了验证。根据费米弧线或类费米弧线的不同行为,边缘模式可分为四类。我们证明了边缘模式不仅存在于等离子体-真空界面,也存在于更一般的等离子体-等离子体界面。这一发现拓宽了这些奇异激发在空间和实验室等离子体中的应用。
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Topological phases, topological phase transition, and bulk-edge correspondence of magnetized cold plasmas
Plasmas have been recently studied as topological materials. We attempt at a comprehensive picture of the topological phases, topological phase transitions, and the bulk-edge correspondence of magnetized cold plasmas. We find that there are 10 topological phases in the parameter space of density $n$, magnetic field $B$, and parallel wavenumber $k_{\parallel}$. They are separated by the surfaces of Langmuir wave-L wave resonance, Langmuir wave-cyclotron wave resonance, and zero magnetic field. For fixed $B$ and $k_{\parallel}$, only the phase transition at the Langmuir wave-cyclotron wave resonance corresponds to edge modes. A sufficient and necessary condition for the existence of this new type of edge modes is given and verified by numerical solutions. The edge modes fall into four categories characterized by different behaviors of the Fermi arcs or Fermi-arcs-like curves. We demonstrate that edge modes exist not only on a plasma-vacuum interface but also on more general plasma-plasma interfaces. This finding broadens the possible applications of these exotic excitations in space and laboratory plasmas.
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