Abstract

Under certain conditions electrons can be reflected and effectively energized at quasi‐perpendicular shocks. This process is most prominent close to the point where the upstream magnetic field is tangent to the curved shock. The energization process has been observed at the Earth's bow shock, but is also considered to occur elsewhere in space. A theoretical explanation of the underlying physical mechanism has been proposed which assumes conservation of magnetic moment and a static, simplified shock profile. We perform test particle calculations of the electron reflection process in order to examine the results of the theoretical analysis without imposing these restrictive conditions. A one‐dimensional hybrid simulation code generates the characteristic field variations across the shock. Special emphasis is placed on the spatial and temporal length scales involved in the mirroring process. The simulation results agree generally well with the predictions from adiabatic theory. The effects of the cross‐shock potential and unsteadiness are quantified, and the influence of field fluctuations on the reflection process is discussed.

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