Wave Generation by Flare-accelerated Ions and Implications for 3He Acceleration

The waves generated by high-energy proton and alpha particles streaming from solar flares into regions of colder plasma are explored using particle-in-cell simulations. Initial distribution functions for the protons and alphas consist of two populations: an energetic, streaming population represente...

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Main Authors: A. Fitzmaurice, J. F. Drake, M. Swisdak
Format: Article
Language:English
Published: IOP Publishing 2024-01-01
Series:The Astrophysical Journal
Subjects:
Online Access:https://doi.org/10.3847/1538-4357/ad217f
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author A. Fitzmaurice
J. F. Drake
M. Swisdak
author_facet A. Fitzmaurice
J. F. Drake
M. Swisdak
author_sort A. Fitzmaurice
collection DOAJ
description The waves generated by high-energy proton and alpha particles streaming from solar flares into regions of colder plasma are explored using particle-in-cell simulations. Initial distribution functions for the protons and alphas consist of two populations: an energetic, streaming population represented by an anisotropic ( T _∥ > T _⊥ ), one-sided kappa function and a cold, Maxwellian background population. The anisotropies and nonzero heat fluxes of these distributions destabilize oblique waves with a range of frequencies below the proton cyclotron frequency. These waves scatter particles out of the tails of the initial distributions along constant-energy surfaces in the wave frame. Overlap of the nonlinear resonance widths allows particles to scatter into near-isotropic distributions by the end of the simulations. The dynamics of ^3 He are explored using test particles. Their temperatures can increase by a factor of nearly 20. Propagation of such waves into regions above and below the flare site can lead to heating and transport of ^3 He into the flare acceleration region. The amount of heated ^3 He that will be driven into the flare site is proportional to the wave energy. Using values from our simulations, we show that the abundance of ^3 He driven into the acceleration region should approach that of ^4 He in the corona. Therefore, waves driven by energetic ions produced in flares are a strong candidate to drive the enhancements of ^3 He observed in impulsive flares.
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spelling doaj.art-2f48466d534941879e8f61d40b126c312024-03-20T09:44:31ZengIOP PublishingThe Astrophysical Journal1538-43572024-01-0196419710.3847/1538-4357/ad217fWave Generation by Flare-accelerated Ions and Implications for 3He AccelerationA. Fitzmaurice0J. F. Drake1https://orcid.org/0000-0002-9150-1841M. Swisdak2https://orcid.org/0000-0002-5435-3544Department of Physics, University of Maryland , College Park, MD 20740, USA; Institute for Research in Electronics and Applied Physics, University of Maryland , College Park, MD 20740, USAInstitute for Research in Electronics and Applied Physics, University of Maryland , College Park, MD 20740, USA; Department of Physics, the Institute for Physical Science and Technology and the Joint Space Institute, University of Maryland , College Park, MD 20740, USADepartment of Physics, University of Maryland , College Park, MD 20740, USA; Institute for Research in Electronics and Applied Physics, University of Maryland , College Park, MD 20740, USAThe waves generated by high-energy proton and alpha particles streaming from solar flares into regions of colder plasma are explored using particle-in-cell simulations. Initial distribution functions for the protons and alphas consist of two populations: an energetic, streaming population represented by an anisotropic ( T _∥ > T _⊥ ), one-sided kappa function and a cold, Maxwellian background population. The anisotropies and nonzero heat fluxes of these distributions destabilize oblique waves with a range of frequencies below the proton cyclotron frequency. These waves scatter particles out of the tails of the initial distributions along constant-energy surfaces in the wave frame. Overlap of the nonlinear resonance widths allows particles to scatter into near-isotropic distributions by the end of the simulations. The dynamics of ^3 He are explored using test particles. Their temperatures can increase by a factor of nearly 20. Propagation of such waves into regions above and below the flare site can lead to heating and transport of ^3 He into the flare acceleration region. The amount of heated ^3 He that will be driven into the flare site is proportional to the wave energy. Using values from our simulations, we show that the abundance of ^3 He driven into the acceleration region should approach that of ^4 He in the corona. Therefore, waves driven by energetic ions produced in flares are a strong candidate to drive the enhancements of ^3 He observed in impulsive flares.https://doi.org/10.3847/1538-4357/ad217fSolar energetic particlesSolar physicsSolar flaresSpace plasmas
spellingShingle A. Fitzmaurice
J. F. Drake
M. Swisdak
Wave Generation by Flare-accelerated Ions and Implications for 3He Acceleration
The Astrophysical Journal
Solar energetic particles
Solar physics
Solar flares
Space plasmas
title Wave Generation by Flare-accelerated Ions and Implications for 3He Acceleration
title_full Wave Generation by Flare-accelerated Ions and Implications for 3He Acceleration
title_fullStr Wave Generation by Flare-accelerated Ions and Implications for 3He Acceleration
title_full_unstemmed Wave Generation by Flare-accelerated Ions and Implications for 3He Acceleration
title_short Wave Generation by Flare-accelerated Ions and Implications for 3He Acceleration
title_sort wave generation by flare accelerated ions and implications for 3he acceleration
topic Solar energetic particles
Solar physics
Solar flares
Space plasmas
url https://doi.org/10.3847/1538-4357/ad217f
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