2020
DOI: 10.3847/1538-4357/abb099
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A Quasi-linear Diffusion Model for Resonant Wave–Particle Instability in Homogeneous Plasma

Abstract: In this paper, we develop a model to describe the generalized wave-particle instability in a quasi-neutral plasma. We analyze the quasi-linear diffusion equation for particles by expressing an arbitrary unstable and resonant wave mode as a Gaussian wave packet, allowing for an arbitrary direction of propagation with respect to the background magnetic field. We show that the localized energy density of the Gaussian wave packet determines the velocityspace range in which the dominant wave-particle instability an… Show more

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Cited by 32 publications
(36 citation statements)
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“…The evolution of the main velocity moments, such as drifting or beaming speeds, and temperature components (parallel and perpendicular to the magnetic field) is confirmed by the numerical simulations, which also show that transient deformations of the distributions fade over time, while their initial shape (e.g., bi-Maxwellian with lower drifts for drifting components) is mainly restored during the relaxation [10,[21][22][23][24]. More elaborate QL diffusion theories attempting to reproduce transient deformations of the anisotropic distribution [25] are however complicated and restricted thus far to a limited approximation of treating the wave spectral intensity as fixed and not evolving in time, which make their implementation to fully describe the saturation of the fluctuations and relaxation of the anisotropic distribution not yet feasible.…”
Section: Introductionsupporting
confidence: 57%
“…The evolution of the main velocity moments, such as drifting or beaming speeds, and temperature components (parallel and perpendicular to the magnetic field) is confirmed by the numerical simulations, which also show that transient deformations of the distributions fade over time, while their initial shape (e.g., bi-Maxwellian with lower drifts for drifting components) is mainly restored during the relaxation [10,[21][22][23][24]. More elaborate QL diffusion theories attempting to reproduce transient deformations of the anisotropic distribution [25] are however complicated and restricted thus far to a limited approximation of treating the wave spectral intensity as fixed and not evolving in time, which make their implementation to fully describe the saturation of the fluctuations and relaxation of the anisotropic distribution not yet feasible.…”
Section: Introductionsupporting
confidence: 57%
“…5) Another possible reason why a strahl may not be detected at 1 AU is because of plasma-wave instabilities that may have disrupted the strahl, (e.g. Gary and Saito, 2007;Kuzichev et al, 2019;Lopez et al, 2019;Vasko et al, 2019;Versharen et al, 2019;Jeong et al, 2020;Micera et al, 2020). Parameterization of instability thresholds is needed and then a matching of strahlchange locations with plasma-parameter changes is needed to test the instability possibility.…”
Section: Discussion: Interpretation Of Strahl-intensity Changes Assementioning
confidence: 99%
“…In the near-Sun solar wind (at ∼34 R S ), Coulomb collisions only effectively scatter the strahl electrons with energies smaller than 250 eV (Horaites et al 2018;Boldyrev & Horaites 2019;. The scattering of the strahl at higher energies and the creation of the halo population are therefore attributed to other phenomena, including waveparticle interactions (Vocks et al 2005;Kajdič et al 2016;Verscharen et al 2019;Jagarlamudi et al 2020;Jeong et al 2020;Cattell et al 2021) and scattering by background turbulence (Pagel et al 2007;Saito & Gary 2007). Observational studies by Štverák et al (2009) and Halekas et al (2020) suggest that the halo is more prominent farther from the Sun, which could be the reason why the sunward deficit has not been observed at larger radial distances (Figure 5(a)).…”
Section: Ambipolar Electric Potential (φ R∞ )mentioning
confidence: 99%