The plasma on an auroral field line is simulated using a Vlasov model. In the initial state, the acceleration region extends from one to three Earth radii in altitude with about half of the acceleration voltage concentrated in a stationary double layer at the bottom of this region. A population of electrons is trapped between the double layer and their magnetic mirror points at lower altitudes. A simulation study is carried out to examine the effects of fluctuations in the total accelerating voltage, which may be due to changes in the generator or the load of the auroral current circuit. The electron distribution function on the high potential side of the double layer changes significantly depending on whether the perturbation...
The current-voltage relationship in the auroral particle acceleration region has been studied stati...
Two auroras sampled nearly simultaneously at high and low altitudes along a field line by the Dynami...
The shift from wave-generated anomalous resistivity toward the more large-scale effects of magnetic ...
The plasma on an auroral field line is simulated using a Vlasov model. In the initial state, the acc...
An auroral flux tube is modelled from the magnetospheric equator to the ionosphere using Vlasov simu...
An auroral flux tube is modelled from the magnetospheric equator to the ionosphere using Vlasov sim...
The plasma on a magnetic field line in the downward current region of the aurora is simulated using ...
Time-stationary solutions to the Vlasov-Poisson equation for ion holes and double layers were examin...
Modern investigations of dynamical space plasma systems such as magnetically complicated topologies ...
[1] The auroral downward field-aligned current is mainly carried by electrons accelerated up from th...
Electric potential-differences between the magnetospheric and the ionospheric end of a magnetic flu...
[1] Satellite observations have established that parallel electric fields of both upward and downwar...
[1] The auroral downward field-aligned current is mainly carried by electrons accelerated up from th...
Electric potential-differences between the magnetospheric and the ionospheric end of a magnetic flux...
Field-aligned currents at Earth's high latitudes are principally carried by accelerated electrons. C...
The current-voltage relationship in the auroral particle acceleration region has been studied stati...
Two auroras sampled nearly simultaneously at high and low altitudes along a field line by the Dynami...
The shift from wave-generated anomalous resistivity toward the more large-scale effects of magnetic ...
The plasma on an auroral field line is simulated using a Vlasov model. In the initial state, the acc...
An auroral flux tube is modelled from the magnetospheric equator to the ionosphere using Vlasov simu...
An auroral flux tube is modelled from the magnetospheric equator to the ionosphere using Vlasov sim...
The plasma on a magnetic field line in the downward current region of the aurora is simulated using ...
Time-stationary solutions to the Vlasov-Poisson equation for ion holes and double layers were examin...
Modern investigations of dynamical space plasma systems such as magnetically complicated topologies ...
[1] The auroral downward field-aligned current is mainly carried by electrons accelerated up from th...
Electric potential-differences between the magnetospheric and the ionospheric end of a magnetic flu...
[1] Satellite observations have established that parallel electric fields of both upward and downwar...
[1] The auroral downward field-aligned current is mainly carried by electrons accelerated up from th...
Electric potential-differences between the magnetospheric and the ionospheric end of a magnetic flux...
Field-aligned currents at Earth's high latitudes are principally carried by accelerated electrons. C...
The current-voltage relationship in the auroral particle acceleration region has been studied stati...
Two auroras sampled nearly simultaneously at high and low altitudes along a field line by the Dynami...
The shift from wave-generated anomalous resistivity toward the more large-scale effects of magnetic ...