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Linear mode conversion of Langmuir/z-mode waves to radiation: Scalings of conversion efficiencies and propagation angles with temperature and magnetic field orientation

机译:Langmuir / z模式波到辐射的线性模式转换:转换效率和传播角随温度和磁场方向的变化比例

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Linear mode conversion (LMC) is the linear transfer of energy from one wave mode to another in an inhomogeneous plasma. It is relevant to laboratory plasmas and multiple solar system radio emissions, such as continuum radiation from planetary magnetospheres and type II and III radio bursts from the solar corona and solar wind. This paper simulates LMC of waves defined by warm, magnetized fluid theory, specifically the conversion of Langmuir/z-mode waves to electromagnetic (EM) radiation. The primary focus is the calculation of the energy and power conversion efficiencies for LMC as functions of the angle of incidence θ of the Langmuir/z-mode wave, temperature β T e / m e c 2, adiabatic index γ, and orientation angle between the ambient density gradient ? N 0 and ambient magnetic field B 0 in a warm, unmagnetized plasma. The ratio of these efficiencies is found to agree well as a function of θ, γ, and β with an analytical relation that depends on the group speeds of the Langmuir/z and EM wave modes. The results demonstrate that the energy conversion efficiency ε is strongly dependent on γ β, and θ, with ε (γ β) 1 / 2 and θ (γ β) 1 / 2. The power conversion efficiency ε p, on the other hand, is independent of γ β but does vary significantly with θ and. The efficiencies are shown to be maximum for approximately perpendicular density gradients (≈ 90 °) and minimal for parallel orientation (0 °) and both the energy and power conversion efficiencies peak at the same θ.
机译:线性模式转换(LMC)是在非均质等离子体中能量从一种波动模式到另一种波动模式的线性传递。它与实验室等离子体和多种太阳系无线电发射有关,例如行星磁层的连续辐射以及太阳日冕和太阳风产生的II型和III型无线电脉冲。本文模拟了由温热磁化流体理论定义的波的LMC,特别是将Langmuir / z模式波转换为电磁(EM)辐射的过程。主要关注点是LMC的能量和功率转换效率的计算,该函数取决于Langmuir / z模波的入射角θ,温度βT e / mec 2,绝热指数γ和环境之间的取向角密度梯度? N 0和周围磁场B 0处于温暖,未磁化的等离子体中。发现这些效率的比率与θ,γ和β的函数非常吻合,并且具有取决于Langmuir / z和EM波模式的群速度的解析关系。结果表明,能量转换效率ε与γβ和θ密切相关,其中ε(γβ)1/2和θ(γβ)1/2。与γβ无关,但随θ和显着变化。对于近似垂直的密度梯度(≈90°),效率显示为最大值;对于平行方向(0°),效率显示为最小,并且能量和功率转换效率均在相同的θ处达到峰值。

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