2014
DOI: 10.5194/angeo-32-507-2014
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Resonant scattering of energetic electrons in the plasmasphere by monotonic whistler-mode waves artificially generated by ionospheric modification

Abstract: Abstract. Modulated high-frequency (HF) heating of the ionosphere provides a feasible means of artificially generating extremely low-frequency (ELF)/very low-frequency (VLF) whistler waves, which can leak into the inner magnetosphere and contribute to resonant interactions with highenergy electrons in the plasmasphere. By ray tracing the magnetospheric propagation of ELF/VLF emissions artificially generated at low-invariant latitudes, we evaluate the relativistic electron resonant energies along the ray paths … Show more

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Cited by 9 publications
(9 citation statements)
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“…We can find that unlike the field‐aligned waves, the profile of diffusion rates of highly oblique waves is very unsmooth, with some pronounced nulls, such as 30°–35°. Actually, this feature has been captured in some previous works regarding to highly oblique waves (Bortnik & Thorne, ; Chang et al, ). Beyond that, Figure shows that the highly oblique monotonic waves can drive pitch angle scattering of 300‐keV electrons with a rate of ~10 −6 /s at low equatorial pitch angles near the loss cone, which is similar to that of field‐aligned monotonic wave in Figure .…”
Section: The Simulation Resultsmentioning
confidence: 80%
“…We can find that unlike the field‐aligned waves, the profile of diffusion rates of highly oblique waves is very unsmooth, with some pronounced nulls, such as 30°–35°. Actually, this feature has been captured in some previous works regarding to highly oblique waves (Bortnik & Thorne, ; Chang et al, ). Beyond that, Figure shows that the highly oblique monotonic waves can drive pitch angle scattering of 300‐keV electrons with a rate of ~10 −6 /s at low equatorial pitch angles near the loss cone, which is similar to that of field‐aligned monotonic wave in Figure .…”
Section: The Simulation Resultsmentioning
confidence: 80%
“…This signal excites a VLF whistler mode resonator supported by amplification by cyclotron resonance with radiation belt particles trapped on the magnetic field lines (Figure 18). The energy of the resonant particles is computed from the cyclotron resonance formula (Chang et al., 2014; Sa, 1989). θt=k1vω1+ωcewhereωce=eB0me,Ee=12mev2. …”
Section: Whistler Mode Propagation In the Magneto‐plasmamentioning
confidence: 99%
“…Typically, only the n = 0, ±1, ±2 resonances need to be considered for Whistler waves; however, sufficiently high-energy electrons may have access to the higher-order resonances (Chang et al 2014). Equation (2.23) may, alternatively, be expressed as: where r rel.…”
Section: Transport Via Magnetic Pitch-angle Diffusionmentioning
confidence: 99%