质子各向同性边界的统计特征

Colin Wilkins, Vassilis Angelopoulos, Anton Artemyev, Andrei Runov, Xiao-Jia Zhang, Jiang Liu, Ethan Tsai
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We find that proton\nIBs are observed under all observed activity levels, spanning 16 to 05 MLT with\n$\\sim$100% occurrence between 19 and 03 MLT, trending toward 60% at dawn/dusk.\nThese results are also compared with electron IB properties observed using\nELFIN, where we find similar trends across local time and activity, with the\nonset in $\\geq$50 keV proton IB occurring on average 2 L-shells lower, and\nproviding between 3 and 10 times as much precipitating power. Proton IBs\ntypically span $64^\\circ$-$66^\\circ$ in magnetic latitude (5-6 in L-shell),\ncorresponding to the outer edge of the ring current, tending toward lower IGRF\nlatitudes as geomagnetic activity increases. The IBs were found to commonly\noccur 0.3-2.1 Re beyond the plasmapause. 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摘要

利用来自 ELFIN 卫星的粒子数据,我们对夜磁层上的 284 个质子各向同性边界事件进行了统计研究,描述了这些事件的发生及其在当地时间、纬度(L 壳)、能量和析出能量通量方面的分布,并将其作为地磁活动的函数。对于给定的带电粒子种类和能量,其各向同性边界(IB)是磁纬度的极向,在该纬度上首次观测到持续的各向同性间距角分布($J_{prec}/J_{perp}\sim 1$)。这种各向同性被解释为赤道磁层的磁场线曲率(FLC)散射所致。我们发现,质子IB在所有观测到的活动水平下都能观测到,时间跨度从16到05 MLT,在19到03 MLT之间质子IB的发生率为100%,在黎明/黄昏时趋向于60%。这些结果还与利用ELFIN观测到的电子IB特性进行了比较,我们发现在不同时间段和不同活动水平下的趋势相似,在$\geq$50 keV质子IB中的起始时间平均低2 L-shells,提供了3到10倍的沉淀能量。质子 IB 通常跨越 64^\circ$-66^\circ$ 的磁纬(5-6 个 L 壳),与环流的外缘相对应,随着地磁活动的增加而趋向于更低的 IGR 纬度。发现IB通常发生在质子停顿期之外0.3-2.1Re处。质子 IB 的能量跨度通常在 50 keV 到 1 MeV 之间,在 22 MLT 附近达到最大,在黎明和黄昏时减小到 300-400 keV 的典型上限,在活跃期观测到的各向同性能量峰值增加了 500 keV。这些结果表明,IB附近的FLC可以为高能质子提供一个重要的耗竭机制,FLC散射产生的总的夜间析出功率约为100 MW,有时为10 GW。
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Statistical Characteristics of the Proton Isotropy Boundary
Using particle data from the ELFIN satellites, we present a statistical study of 284 proton isotropy boundary events on the nightside magnetosphere, characterizing their occurrence and distribution in local time, latitude (L-shell), energy, and precipitating energy flux, as a function of geomagnetic activity. For a given charged particle species and energy, its isotropy boundary (IB) is the magnetic latitude poleward of which persistently isotropic pitch-angle distributions ($J_{prec}/J_{perp}\sim 1$) are first observed to occur. This isotropization is interpreted as resulting from magnetic field-line curvature (FLC) scattering in the equatorial magnetosphere. We find that proton IBs are observed under all observed activity levels, spanning 16 to 05 MLT with $\sim$100% occurrence between 19 and 03 MLT, trending toward 60% at dawn/dusk. These results are also compared with electron IB properties observed using ELFIN, where we find similar trends across local time and activity, with the onset in $\geq$50 keV proton IB occurring on average 2 L-shells lower, and providing between 3 and 10 times as much precipitating power. Proton IBs typically span $64^\circ$-$66^\circ$ in magnetic latitude (5-6 in L-shell), corresponding to the outer edge of the ring current, tending toward lower IGRF latitudes as geomagnetic activity increases. The IBs were found to commonly occur 0.3-2.1 Re beyond the plasmapause. Proton IBs typically span $<$50 keV to $\sim$1 MeV in energy, maximizing near 22 MLT, and decreasing to a typical upper limit of 300-400 keV toward dawn and dusk, with peak observed isotropic energy increasing by $\sim$500 keV during active intervals. These results suggest that FLC in the vicinity of IBs can provide a substantial depletion mechanism for energetic protons, with the total nightside precipitating power from FLC-scattering found to be on the order of 100 MW, at times $\geq$10 GW.
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