Linear stability analysis of magnetized relativistic jets: the non-rotating case
Linear stability analysis of magnetized relativistic jets: the non-rotating case
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磁化相对论射流的线性稳定性分析:非旋转情况
DOI:
10.1093/mnras/stt1225
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发表时间:
2013
影响因子:
4.8
通讯作者:
Andrea Mignone
中科院分区:
文献类型:
--
作者:
G. Bodo;G. Mamatsashvili;P. Rossi;Andrea Mignone
We perform a linear analysis of the stability of a magnetized relativistic nonrotating cylindrical flow in the aproximation of zero thermal pressure, considering only the |m| = 1 mode. We find that there are two modes of instability: Kelvin-Helmholtz and current driven. The Kelvin-Helmholtz mode is found at low magnetizations and its growth rate depends very weakly on the pitch parameter. The current driven modes are found at high magnetizations and the value of the growth rate and the wavenumber of the maximum increase as we decrease the pitch parameter. In the relativistic regime the current driven mode is splitted in two branches, the branch at high wavenumbers is characterized by the eigenfunction concentrated in the jet core, the branch at low wavenumbers is instead characterized by the eigenfunction that extends outside the jet velocity shear region. The formation and propagation of astrophysical jets are strongly affected by plasma instabilities, whose study is therefore of fundamental importance for understanding their dynamics and their associated phenomenology. In jets there are several possible different kinds of instability, among them the most studied are the Kelvin-Helmholtz instability (KHI) driven by the velocity shear between the jet and the ambient medium and the current driven instability (CDI) associated with a longitudinal current and therefore with the toroidal component of magnetic field. Since the most promising models for the acceleration and collimation of jets involve the presence of a magnetic field with footpoints anchored to a rotating object (an accretion disk or a spinning star or black hole), the presence of a toroidal field component is a