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)