SH008-08
Shock Acceleration of ~1-100 Kev Electrons at Earth`s Bow Shock I

Tuesday, 8 December 2020: 04:44
Virtual
Zixuan Liu1, Linghua Wang1, Quanqi Shi2, Liu Yang3, Robert F Wimmer-Schweingruber4 and Stuart D Bale5, (1)Peking University, Beijing, China, (2)Shandong University at Weihai, Weihai, China, (3)Peking University, Institute of Space Physics and Applied Technology, Beijing, China, (4)University of Kiel, Institute for Experimental and Applied Physics, Kiel, Germany, (5)University of California Berkeley, Space Sciences Laboratory, Berkeley, CA, United States
Abstract:
We present a statistical study of shock acceleration of ~1-100 keV solar wind suprathermal eletrons at Earth’s bow shock, by using Wind 3D plasma and energetic particle measurements in ambient solar wind and Magnetospheric Multiscale mission measurements in shock downstream. Among 74 shock cases (1 quasi-parallel shock, 73 quasi-perpendicular shocks) during 2015 October - 2017 January, there are 23 (type 0) without significant electron acceleration after shock passage, 24 (type 1) with power-law-spectrum, J∝W-β1, at ~1-3 keV in downstream, 16 (type 2) with power-law-spectrum at the same energy range and significant flux enhancement above 30 keV in downstream, and 11 (type3) with a clear double-power-law spectrum, J∝W-β1 (J∝W-β2) when W>>Wtr (W<<Wtr), bending down at Wtr~20-90 keV in downstream. The spectral indexes at ~1-3 keV, β1, range from 2.5 to 5, while the spectral indexes above 30 keV, β2, range from 5 to 9, and all the spectral indexes shows no correlation with those in ambient solar wind. To explain the formation of double-power-law spectrum in downstream of type 3 shocks, we use shock drift acceleration model and find that the drift time Td of suprathermal electrons in shock ramp is close to the transmission time Ttr of bulk plasma traveling through shock ramp, Td/Ttr~1-3 (~0.5-1) when W<Wtr (W>Wtr) , and the gyration scale of electrons at Wtr, Dg(Wtr), is close to the ramp thickness Dramp. Besides, Td/Ttr increases (decreases) with energy at W>>Wtr (W<<Wtr), which can lead to a flattened (steepened) energy spectrum in downstream. All of these make a quantitative explanation of the formation of double-power-law spectrum in shock downstream.