Whistler Fan Instability Driven by Strahl Electrons in the Solar Wind
Abstract
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Whistler Fan Instability Driven by Strahl Electrons in the Solar Wind
I. Y. Vasko1,2
, V. Krasnoselskikh1,3, Y. Tong1,4, S. D. Bale1,4
, J. W. Bonnell1, and F. S. Mozer1
Published 2019 January 31 • © 2019. The American Astronomical Society. All rights reserved.
The Astrophysical Journal Letters, Volume 871, Number 2
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Author affiliations
1 Space Sciences Laboratory, University of California, Berkeley, CA 94720, USA
2 Space Research Institute of Russian Academy of Sciences, Moscow, 177997, Russia
3 LPC2E/CNRS, Orlean, France
4 Physics Department, University of California, Berkeley, CA 94720, USA
ORCID iDs
I. Y. Vasko
https://orcid.org/0000-0002-4974-4786
V. Krasnoselskikh
https://orcid.org/0000-0002-6809-6219
Y. Tong
https://orcid.org/0000-0002-3354-486X
S. D. Bale
https://orcid.org/0000-0002-1989-3596
Dates
Received 2019 January 18
Accepted 2019 January 24
Published 2019 January 31
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Citation
I. Y. Vasko et al 2019 ApJL 871 L29
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DOI
https://doi.org/10.3847/2041-8213/ab01bd
Keywords
conduction; instabilities; plasmas; scattering; solar wind; waves
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Abstract
We present a theoretical analysis of electron heat flux inhibition in the solar wind when a significant portion of the heat flux is carried by strahl electrons. We adopt core-strahl velocity distribution functions typical for the solar wind at 0.3–4 au to demonstrate that strahl electrons are capable of generating highly oblique whistler waves at wave numbers kρe ~ 1, where ρe is typical thermal electron gyroradius. The whistler waves are driven by electrons in the anomalous cyclotron resonances (the fan instability) and propagate at typical angles of about 70°–80° to the strahl that is usually anti-sunward. The group velocity of the whistler waves is predominantly parallel to the strahl, thereby facilitating efficient scattering of strahl electrons. We suggest that the highly oblique whistler waves drive pitch-angle scattering of strahl electrons, resulting in halo formation and suppressing the heat flux of strahl electrons below a threshold that is shown to depend on βe . The proposed fan instability is fundamentally different from the whistler heat flux instability driven by the normal cyclotron resonance with halo electrons and being ineffective in suppressing the heat flux of the strahl.