The electron distribution function downstream of the solar-wind termination shock: Where are the hot electrons?

被引:26
作者
Fahr, Hans J. [1 ]
Richardson, John D. [2 ]
Verscharen, Daniel [3 ]
机构
[1] Univ Bonn, Argelander Inst Astron, D-53121 Bonn, Germany
[2] MIT, Kavli Inst Astrophys & Space Res, Cambridge, MA 02139 USA
[3] Univ New Hampshire, Ctr Space Sci, Durham, NH 03824 USA
关键词
plasmas; Sun: heliosphere; solar wind; shock waves; instabilities; COLLISIONLESS-SHOCK; PLASMA; HELIOSHEATH; EQUILIBRIUM; HELIOSPHERE; IONS; JUMP;
D O I
10.1051/0004-6361/201525710
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
In the majority of the literature on plasma shock waves, electrons play the role of "ghost particles", since their contribution to mass and momentum flows is negligible, and they have been treated as only taking care of the electric plasma neutrality. In some more recent papers, however, electrons play a new important role in the shock dynamics and thermodynamics, especially at the solar-wind termination shock. They react on the shock electric field in a very specific way, leading to suprathermal nonequilibrium distributions of the downstream electrons, which can be represented by a kappa distribution function. In this paper, we discuss why this anticipated hot electron population has not been seen by the plasma detectors of the Voyager spacecraft downstream of the solar-wind termination shock. We show that hot nonequilibrium electrons induce a strong negative electric charge-up of any spacecraft cruising through this downstream plasma environment. This charge reduces electron fluxes at the spacecraft detectors to nondetectable intensities. Furthermore, we show that the Debye length lambda(K)(D) grows to values of about lambda(K)(D)/lambda(K)(D) similar or equal to 10(6) compared to the classical value lambda(D) in this hot-electron environment. This unusual condition allows for the propagation of a certain type of electrostatic plasma waves that, at very large wavelengths, allow us to determine the effective temperature of the suprathermal electrons directly by means of the phase velocity of these waves. At moderate wavelengths, the electron-acoustic dispersion relation leads to nonpropagating oscillations with the ion-plasma frequency omega(p), instead of the traditional electron plasma frequency.
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页数:5
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