2017
DOI: 10.1002/2016ja023546
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Magnetospheric whistler mode ray tracing in a warm background plasma with finite electron and ion temperature

Abstract: Whistler mode waves play a major role in the energy dynamics of the Earth's magnetosphere. Numerical ray tracing has been used for many years to determine the propagation trajectories of whistler mode waves from various sources, both natural and anthropogenic. Previous work has been under the ideal cold plasma assumption even though temperatures of the background ions and electrons are in the range of several eV. We perform numerical ray tracing with the inclusion of finite electron and ion temperatures to mor… Show more

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Cited by 18 publications
(18 citation statements)
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References 48 publications
(91 reference statements)
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“…Therefore, the secondary electron outflow can alter whistler mode wave propagation and trigger a ducted propagation of quasiparallel waves. This effect could potentially explain the large number of quasiparallel whistler mode waves observed at relatively high latitudes, at 20–40° (Agapitov et al, 2013; Santolík et al, 2014), where models of nonducted wave propagation predict a dominance of very oblique waves (Breuillard et al, 2012, 2013; Maxworth & Golkowski, 2017; Yamaguchi et al, 2013).…”
Section: Discussionmentioning
confidence: 99%
“…Therefore, the secondary electron outflow can alter whistler mode wave propagation and trigger a ducted propagation of quasiparallel waves. This effect could potentially explain the large number of quasiparallel whistler mode waves observed at relatively high latitudes, at 20–40° (Agapitov et al, 2013; Santolík et al, 2014), where models of nonducted wave propagation predict a dominance of very oblique waves (Breuillard et al, 2012, 2013; Maxworth & Golkowski, 2017; Yamaguchi et al, 2013).…”
Section: Discussionmentioning
confidence: 99%
“…Depending on actual wave properties controlled by the hot plasma dispersion (e.g., Sazhin, ), electron scattering rates due to very oblique waves may increase as compared with quasi‐parallel waves and become very large or else drop down to zero (see discussions in Albert, ; Artemyev et al, ). The critical characteristics determining the total effect of highly oblique chorus waves on resonant electrons are the maximum value N max of the wave refractive index defined by hot plasma effects and/or Landau damping (see Hashimoto et al, ; Horne & Sazhin, ; Kulkarni et al, ; Li et al, ; Maxworth & Golkowski, ; Mourenas et al, ) and the distribution of magnetic wave power near the resonance cone (e.g., Artemyev et al, ; Albert, , and references therein). Both these characteristics can be derived only from a very careful analysis of sufficiently accurate wave, plasma, and electron distribution measurements during very oblique chorus wave observations, allowed for the first time by the Van Allen Probes mission.…”
Section: Introductionmentioning
confidence: 99%
“…The background plasmasphere consists of electron and ions (H + , He + and O + ). This raytracer was later modified at the University of Colorado Denver, to have the option of including finite electron and ion temperature [51]. The background plasma densities used in this work were from the Global Core Plasmasphere Model (GCPM) [55].…”
Section: Raytracing Resultsmentioning
confidence: 99%