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首页> 外文期刊>Physics and chemistry of the earth, Part C. Solar-terrestrial and planetary science >Enhanced Pitch Angle Scattering of Protons at Mid-Latitudes During Geomagnetic Storms
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Enhanced Pitch Angle Scattering of Protons at Mid-Latitudes During Geomagnetic Storms

机译:地磁风暴期间中纬度质子的增强俯仰角散射

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During geomagnetic storms highly localized regions of enhanced proton (ion) precipitation in the tens to several hundred keV energy range can appear at mid-latitudes. The particle pitch angle distribution in these enhanced regions is anisotropic with maximum intensity perpendicular to the magnetic field. In a few cases, however, the distribution can approach isotropy. These regions typically have widths of a few degrees invariant latitude, but can be as narrow as 0.25 deg. The intensity peak is most often concentrated in a specific particle energy range, although in many cases the intensity peak at a given location is distributed over a broader energy range. During the main phase of the storms the ion enhancement is mostly observed in the highest energy protons and only in the midnight/evening MLT sector. Coincident with the ion enhancement there was often an enhancement in electrons with energies > 300 keV. In the recovery phase of the storms the ion enhancement can be observed at all local times covered by our observations and there was not any coincident enhancement in the high energy electrons. Overall the observations seem to support a picture where scattering of protons into the loss cone by cyclotron resonant wave-particle interaction occurs, while high energy electrons are parasitically scattered into the loss cone by the same ion cyclotron waves. Throughout the storm the L-dependence of the enhancements in proton fluxes is similar to the K_p dependence of the location of the plasmapause. Whenever a direct comparison could be made, the SAR arc and the ion enhancement overlap. Thus the ion enhancement and SAR arc are associated, but not necessarily on a cause-effect basis.
机译:在地磁风暴期间,中纬度会出现几十到几百keV能量范围内高度局部化的质子(离子)沉淀增强区域。这些增强区域中的粒子俯仰角分布是各向异性的,其最大强度垂直于磁场。但是,在少数情况下,分布可能接近各向同性。这些区域的宽度通常为几度不变纬度,但可以窄至0.25度。强度峰通常集中在特定的粒子能量范围内,尽管在许多情况下,给定位置的强度峰分布在较宽的能量范围内。在暴风雨的主要阶段,离子增强主要在能量最高的质子中观察到,并且仅在午夜/傍晚的MLT区域中观察到。与离子增强同时发生的是,能量大于300 keV的电子通常会增强。在风暴的恢复阶段,我们观察到的所有局部时间都可以观察到离子增强,并且高能电子没有任何同时的增强。总的来说,这些观察结果似乎支持了这样的情况:质子通过回旋共振波-粒子相互作用而发生质子散射进入损耗锥,而高能电子被相同的离子回旋波寄生地散射到损耗锥中。在整个风暴中,质子通量增强的L相关性与等离子停顿位置的K_p相关性相似。只要可以进行直接比较,SAR电弧和离子增强就会重叠。因此,离子增强和SAR电弧相关联,但不一定基于因果关系。

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