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Magneto-acoustic waves in a gravitationally stratified magnetized plasma: eigen-solutions and their applications to the solar atmosphere

机译:重力分层磁化等离子体中的磁声波:本征解及其在太阳大气中的应用

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摘要

Magneto-acoustic gravity (MAG) waves have been studied intensively in the context of astrophysical plasmas. There are three popular choices of analytic modeling using a Cartesian coordinate system: a magnetic field parallel, perpendicular, or at an angle to the gravitational field. Here, we study a gravitationally stratified plasma embedded in a parallel, so called vertical, magnetic field. We find a governing equation for the auxiliary quantity Θ = p 1/ρ 0, and find solutions in terms of hypergeometric functions. With the convenient relationship between Θ and the vertical velocity component, v z , we derive the solution for v z . We show that the four linearly independent functions for v z can also be cast as single hypergeometric functions, rather than the Frobenius series derived by Leroy & Schwartz. We are then able to analyze a case of approximation for a one-layer solution, taking the small wavelength limit. Motivated by solar atmospheric applications, we finally commence study of the eigenmodes of perturbations for a two-layer model using our solutions, solving the dispersion relation numerically. We show that, for a transition between a photospheric and chromospheric plasma embedded in a vertical magnetic field, modes exist that are between the observationally widely investigated three and five minute oscillation periods, interpreted as solar global oscillations in the lower solar atmosphere. It is also shown that, when the density contrast between the layers is large (e.g., applied to photosphere/chromosphere-corona), the global eigenmodes are practically a superposition of the same as in each of the separate one-layer systems.
机译:在天体物理等离子体的背景下,对磁声重力(MAG)波进行了深入研究。使用笛卡尔坐标系的解析模型有三种流行的选择:平行,垂直或与重力场成一定角度的磁场。在这里,我们研究了嵌入平行磁场(称为垂直磁场)中的重力分层等离子体。我们找到辅助量Θ= p 1 /ρ0的控制方程,并根据超几何函数找到解。利用Θ和垂直速度分量v z之间的便利关系,我们得出v z的解。我们证明v z的四个线性独立函数也可以转换为单个超几何函数,而不是Leroy&Schwartz导出的Frobenius系列。然后,我们可以采用较小的波长限制来分析单层解决方案的近似情况。受太阳大气应用的推动,我们最终开始使用我们的解决方案研究两层模型的摄动本征模,从而数值求解色散关系。我们表明,对于在垂直磁场中嵌入的光球和色球等离子之间的过渡,存在着模式,该模式介于被广泛观察的三到五分钟振荡周期之间,被解释为较低太阳大气中的太阳全局振荡。还显示出,当各层之间的密度对比度大时(例如,应用于光球/色球层电晕),总体本征模式实际上是与每个单独的单层系统相同的叠加。

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    Mather J.F.; Erdélyi R.;

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  • 年度 2016
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