The effect of a non-maxwellian electron velocity distribution on Be-like ion diagnostics in the Sun

Solar Physics ◽  
1984 ◽  
Vol 91 (1) ◽  
Author(s):  
F.P. Keenan
1977 ◽  
Vol 43 ◽  
pp. 28-28
Author(s):  
J. L. Linsky

This paper wil describe recent calculations which attempt to pin down the relative importance of collisional excitation, recombination, diffusion, and departures from a Maxwell-Boltzmann electron velocity distribution on the formation of lines and continua of He I and He II in the Sun. There will be some comments on the relevance of these calculations to other stars.


2021 ◽  
Author(s):  
Alfredo Micera ◽  
Andrei Zhukov ◽  
Rodrigo A. López ◽  
Maria Elena Innocenti ◽  
Marian Lazar ◽  
...  

<p>Electron velocity distribution functions, initially composed of core and strahl populations as typically encountered in the near-Sun solar wind and as recently observed by Parker Solar Probe, have been modeled via fully kinetic Particle-In-Cell simulations. It has been demonstrated that, as a consequence of the evolution of the electron velocity distribution function, two branches of the whistler heat flux instability can be excited, which can drive whistler waves propagating in the direction parallel or oblique to the background magnetic field. First, the strahl undergoes pitch-angle scattering with oblique whistler waves, which provokes the reduction of the strahl drift velocity and the simultaneous broadening of its pitch angle distribution. Moreover, the interaction with the oblique whistler waves results in the scattering towards higher perpendicular velocities of resonant strahl electrons and in the appearance of a suprathermal halo population which, at higher energies, deviates from the Maxwellian distribution. Later on, the excited whistler waves shift towards smaller angles of propagation and secondary scattering processes with quasi-parallel whistler waves lead to a redistribution of the scattered particles into a more symmetric halo. All processes are accompanied by a significant decrease of the heat flux carried by the strahl population along the magnetic field direction, although the strongest heat flux rate decrease is simultaneous with the propagation of the oblique whistler waves.</p>


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