Electron heating and electron-ion temperature ratio at shocks · revision history

Revision 1

Accepted · first revision · record

Title
Electron heating and electron-ion temperature ratio at shocks
Plain
Behind fast shocks in supernova remnants, electrons end up much colder than ions, while behind slow shocks the two are similar. Which processes heat electrons inside a collisionless shock is not known.
Precise
Balmer-line observations of supernova remnant shocks show downstream $T_{\mathrm{e}}/T_{\mathrm{i}}$ near 1 at low shock speed and well below 1 at high speed. Identify the electron heating mechanism (cross-shock potential, wave heating by Buneman or whistler instabilities, reconnection in the shock transition) and derive $T_{\mathrm{e}}/T_{\mathrm{i}}$ versus Mach number and obliquity. An answer is a derived relation matching observations and kinetic simulations.
Settled by
Kinetic simulations at realistic mass ratio reproducing the observed $T_{\mathrm{e}}/T_{\mathrm{i}}$ trend, with the mechanism identified.
Kind
phenomenon
Answer type
mechanism
References
(empty)
Literature status
open
Status note
(empty)
Posed since
(empty)