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首页> 外文期刊>The Astrophysical journal >RADIAL STREAMING ANISOTROPIES OF CHARGED PARTICLES ACCELERATED AT THE SOLAR WIND TERMINATION SHOCK
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RADIAL STREAMING ANISOTROPIES OF CHARGED PARTICLES ACCELERATED AT THE SOLAR WIND TERMINATION SHOCK

机译:太阳风终止冲击时带电粒子的径向条纹各向异性

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摘要

Recent observations of an increase in energetic particle intensities on the Voyager 1 spacecraft, for several months in late 2002 to early 2003, suggest new phenomena associated with its approach to the termination shock of the solar wind. An important diagnostic used by the experimenters to interpret the event has been the radial anisotropy of the energetic particle distribution. In this Letter we consider the transport of energetic charged particles accelerated at the termination shock, both in the diffusion approximation and by directly integrating test particle trajectories in a turbulent magnetic field. We determine the radial anisotropy in a number of models. In general, we find that the radial anisotropy of the particles is complicated and that it cannot reliably be used to determine the radial velocity of the background plasma. In all cases considered, we find that the average radial anisotropy in the region upstream of the shock is directed toward the shock and is less than or equal to the Compton-Getting anisotropy in the slower wind downstream. We attribute the difference from the Compton-Getting anisotropy to the diffusive anisotropy, which is directed upstream away from the shock and which is part of the acceleration process. We suggest that the small radial anisotropy observed on Voyager 1 at low energies may actually be an indication that Voyager 1 was located upstream of the shock during the entire event. In addition, we find large fluctuating anisotropies along the magnetic field (nearly transverse to the radial direction).
机译:在2002年底至2003年初的几个月中,最近对Voyager 1航天器的高能粒子强度增加的观察表明,新的现象与其处理太阳风的终止冲击有关。实验人员用来解释该事件的重要诊断方法是高能粒子分布的径向各向异性。在这封信中,我们考虑了在扩散激波中以及通过直接将测试粒子的轨迹整合到湍流磁场中而在终止冲击时加速的高能带电粒子的传输。我们在许多模型中确定了径向各向异性。通常,我们发现粒子的径向各向异性很复杂,无法可靠地用于确定背景等离子体的径向速度。在所有考虑的情况下,我们发现冲击上游区域的平均径向各向异性是指向冲击的,并且小于或等于下游较慢风中的康普顿-各向异性。我们将不同于Compton-Getting各向异性的原因归因于扩散各向异性,该扩散各向异性指向远离冲击的上游,并且是加速过程的一部分。我们建议在低能量的旅行者1号上观察到较小的径向各向异性,这实际上可能表明旅行者1号在整个事件中位于激波的上游。另外,我们发现沿磁场(几乎垂直于径向)的大的波动各向异性。

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