The firehose instability is driven by a pressure anisotropy in a magnetized plasma when the plasma has T??? > T???, that is, the temperature along the magnetic field is higher than the perpendicular temperature. Such condition occurs commonly in astrophysical and space environments, for instance, when there are beams aligned with the background magnetic field. Recently, it was argued that around weak quasi-perpendicular shocks in high-?? plasmas of the intracluster medium, shock-reflected electrons propagating upstream cause the temperature anisotropy of T??? > T???. This electron temperature anisotropy can trigger the electron firehose instability (EFI). In the study, the kinetic properties of the EFI are first examined by the linear...
The preacceleration of electrons through reflection and shock drift acceleration (SDA) is essential ...
The isotropization process of a collisionless plasma with an electron temperature anisotropy along a...
Electron acceleration to non-thermal energies is known to occur in low Mach number (Ms. 5) shocks in...
© 2019 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Societ...
Self-generated wave fluctuations are particularly interesting in the solar wind and magnetospheric p...
Electromagnetic instabilities in high-β plasmas, where β is the ratio of the kinetic plasma energy t...
Context. Recent studies have revealed new unstable regimes of the counter-beaming electrons specific...
In coronal outflows and solar winds, the presence of the interplanetary magnetic field and heat flux...
We report the first results from particle-in-cell simulations of the fast-growing aperiodic electron...
The increase of temperature predicted by the solar wind expansion in the direction parallel to the i...
The double adiabatic expansion of the nearly collisionless solar wind plasma creates conditions for ...
Among the kinetic microinstabilities, the firehose instability is one of the most efficient mechanis...
Firehose-like instabilities (FIs) are cited in multiple astrophysical applications. Of particular in...
Weakly collisional plasmas dynamically develop pressure anisotropies with respect to the magnetic fi...
Electron acceleration to non-thermal energies is known to occur in low Mach number (Ms 5) shocks in...
The preacceleration of electrons through reflection and shock drift acceleration (SDA) is essential ...
The isotropization process of a collisionless plasma with an electron temperature anisotropy along a...
Electron acceleration to non-thermal energies is known to occur in low Mach number (Ms. 5) shocks in...
© 2019 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Societ...
Self-generated wave fluctuations are particularly interesting in the solar wind and magnetospheric p...
Electromagnetic instabilities in high-β plasmas, where β is the ratio of the kinetic plasma energy t...
Context. Recent studies have revealed new unstable regimes of the counter-beaming electrons specific...
In coronal outflows and solar winds, the presence of the interplanetary magnetic field and heat flux...
We report the first results from particle-in-cell simulations of the fast-growing aperiodic electron...
The increase of temperature predicted by the solar wind expansion in the direction parallel to the i...
The double adiabatic expansion of the nearly collisionless solar wind plasma creates conditions for ...
Among the kinetic microinstabilities, the firehose instability is one of the most efficient mechanis...
Firehose-like instabilities (FIs) are cited in multiple astrophysical applications. Of particular in...
Weakly collisional plasmas dynamically develop pressure anisotropies with respect to the magnetic fi...
Electron acceleration to non-thermal energies is known to occur in low Mach number (Ms 5) shocks in...
The preacceleration of electrons through reflection and shock drift acceleration (SDA) is essential ...
The isotropization process of a collisionless plasma with an electron temperature anisotropy along a...
Electron acceleration to non-thermal energies is known to occur in low Mach number (Ms. 5) shocks in...