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Simulation study of the whistler-mode chorus generation in the Earth's inner magnetosphere

机译:地球内磁层中吹口石模式的仿真研究

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Whistler-mode chorus emissions play crucial roles in the evolution of radiation belt electrons. Chorus emissions are coherent electromagnetic plasma waves with varying frequencies in the typical frequency range of 0.2 to 0.8 fce0, where fce0 is the electron gyrofrequency at the magnetic equator. They often have a gap at half the local cyclotron frequency. The generation process of chorus has been explained by the nonlinear wave growth theory [see review by Omura et al., 2012] and has been reproduced by self-consistent numerical experiments [e.g., Katoh and Omura, 2007, 2011, 2013, 2016; Katoh et al., 2018]. In the present study, we investigate dependencies of the chorus generation process on properties of energetic electrons, the background magnetic field, and the thermal plasma condition. First, we conduct a series of electron hybrid simulations for different temperature anisotropy (AT) of the initial velocity distribution function of energetic electrons. We vary AT in the range from 3 to 9 with changing the number density of energetic electrons (Nh) so as to study whether distinct rising-tone chorus emissions are reproduced or not in the assumed initial condition. Simulation results reveal that Nh required for the chorus generation decreases as the temperature anisotropy of energetic electrons increases. We also find that reproduced spectra become hiss-like for large Nh cases. Next, we carry out simulations by changing the spatial gradient of the background magnetic field intensity along a field line. Simulation results clarify that the small magnetic field gradient lowers the threshold amplitude for the chorus generation. These simulation results demonstrate the validity of the nonlinear wave growth theory and suggest that the coherent nonlinear wave-particle interaction is essential for generation of whistler-mode chorus emissions in the magnetosphere.
机译:惠斯勒模式合唱排放在辐射带电子的演变中起着至关重要的作用。合唱排放是具有0.2至0.8 f的典型频率范围内具有不同频率的相干电磁等离子体波 ce0 ,其中f ce0 是磁性赤道的电子电磁谱。它们通常在局部回旋频的一半处具有间隙。非线性波长理论解释了合唱的生成过程[查看Omula等人,2012]并已被自我一致的数值实验复制[例如,Katoh和Omura,2007,2007,2013,2016; Katoh等人,2018]。在本研究中,我们研究了合唱生成过程的依赖性对能量电子,背景磁场和热等离子体条件的性质。首先,我们对能量电子的初始速度分布函数的不同温度各向异性(AT)进行一系列电子混合模拟。我们在3到9的范围内变化,改变了能量电子(NH)的数量密度,以研究是否在假定的初始条件下再现了不同的上升音调合唱声排放。仿真结果表明,随着活性电子的温度各向异性增加,合唱生成所需的NH减小。我们还发现复制的光谱变得像大NH案例一样的嘶嘶声。接下来,我们通过沿着场线改变背景磁场强度的空间梯度来执行模拟。仿真结果阐明了小磁场梯度降低了合唱生成的阈值幅度。这些仿真结果表明了非线性波生长理论的有效性,并表明相干非线性波粒子相互作用对于在磁层中产生吹口石模式合唱辐射至关重要。

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