• DOI:10.1093/mnras/stx2555
• Corpus ID: 119457295

Kinetic Theory and Fast Wind Observations of the Electron Strahl

@article{Horaites2017KineticTA,
  title={Kinetic Theory and Fast Wind Observations of the Electron Strahl},
  author={Konstantinos Horaites and Stanislav Boldyrev and Lynn Bruce Wilson and Adolfo. F. Vi{\~n}as and Jan Merka},
  journal={Monthly Notices of the Royal Astronomical Society},
  year={2017},
  volume={474},
  pages={115-127}
}

• K. Horaites, S. Boldyrev, +2 authors J. Merka
• Published 12 June 2017
• Physics
• Monthly Notices of the Royal Astronomical Society

We develop a model for the strahl population in the solar wind -- a narrow, low-density and high-energy electron beam centered on the magnetic field direction. Our model is based on the solution of the electron drift-kinetic equation at heliospheric distances where the plasma density, temperature, and the magnetic field strength decline as power-laws of the distance along a magnetic flux tube. Our solution for the strahl depends on a number of parameters that, in the absence of the analytic solution for the full electron velocity distribution function (eVDF), cannot be derived from the theory. We however demonstrate that these parameters can be efficiently found from matching our solution with observations of the eVDF made by the Wind satellite's SWE strahl detector. The model is successful at predicting the angular width (FWHM) of the strahl for the Wind data at 1 AU, in particular by predicting how this width scales with particle energy and background density. We find the strahl distribution is largely determined by the local temperature Knudsen number $\gamma \sim |T dT/dx|/n$, which parametrizes solar wind collisionality. We compute averaged strahl distributions for typical Knudsen numbers observed in the solar wind, and fit our model to these data. The model can be matched quite closely to the eVDFs at 1 AU, however, it then overestimates the strahl amplitude at larger heliocentric distances. This indicates that our model may be improved through the inclusion of additional physics, possibly through the introduction of "anomalous diffusion" of the strahl electrons.