2021
DOI: 10.1134/s001679322108020x
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Spatio-temporal Dynamics of Fast Electrons and Plasma Turbulence in an Inhomogeneous Flare Plasma

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Cited by 6 publications
(4 citation statements)
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“…Such a pitch‐angle reflection from the loss cone has been found by Inan et al. (1978), Lundin & Shkliar (1977) and described for EMIC waves in Grach and Demekhov (2020) as force bunching . This pitch‐angle increase is described by the second term on the right‐hand side of Equation : the direct influence of Lorentz force on the particle phase is strong for small p ⊥ and can exceed the inertial (or kinematic) bunching effect ∼Δ, the first term in Equation .…”
Section: Simulation Setup and Resultssupporting
confidence: 60%
See 1 more Smart Citation
“…Such a pitch‐angle reflection from the loss cone has been found by Inan et al. (1978), Lundin & Shkliar (1977) and described for EMIC waves in Grach and Demekhov (2020) as force bunching . This pitch‐angle increase is described by the second term on the right‐hand side of Equation : the direct influence of Lorentz force on the particle phase is strong for small p ⊥ and can exceed the inertial (or kinematic) bunching effect ∼Δ, the first term in Equation .…”
Section: Simulation Setup and Resultssupporting
confidence: 60%
“…Electrons with small initial pitch angles show a significant 〈Δα eq 〉 > 0 at the resonant energy that increases with time (with the resonant latitudes where the wave-packet intensity maximizes) from 1 to 1.5 MeV (see red regions in Figure 3e). Such a pitch-angle reflection from the loss cone has been found by Inan et al (1978), Lundin & Shkliar (1977) and described for EMIC waves in Grach and Demekhov (2020) as force bunching. This pitch-angle increase is described by the second term on the right-hand side of Equation 3: the direct influence of Lorentz force on the particle phase is strong for small p ⊥ and can exceed the inertial (or kinematic) bunching effect ∼Δ, the first term in Equation 3.…”
Section: Simulation Setup and Resultsmentioning
confidence: 61%
“…Figures 3e, 3f, 4e, and 4f show that force bunching (Bortnik et al., 2022; Grach & Demekhov, 2020; Grach et al., 2021, 2022; Kitahara & Katoh, 2019; Lundin & Shkliar, 1977) is effective at E=EminSD $E={E}_{\text{min}}^{\text{SD}}$EmaxSD ${E}_{\text{max}}^{\text{SD}}$: precipitation from small pitch angles near the loss cone is substituted by precipitation of electrons at higher α eq0 (see discussions in Grach et al., 2022; Hanzelka, Li, & Ma, 2023), which are precipitated due to interactions in the linear regime, with possible contributions from nonlinear phase trapping that is less effective for shorter packets (see discussions in Grach et al., 2022).…”
Section: Simulation Setup and Resultsmentioning
confidence: 99%
“…The theoretical model for generation of harmonic emissions of Type III solar radio bursts in strongly inhomogeneous plasmas is proposed in [37]. In work [38], the evolution of the electron distribution function and the spectral energy density of Langmuir turbulence with a pulsed injection of electrons in an inhomogeneous flare plasma is studied.…”
Section: Introductionmentioning
confidence: 99%