Nonlinear mechanisms of lower-band and upper-band VLF chorus emissions in the magnetosphere
By Yoshiharu Omura, M. Hikishima, Yuto Katoh, Danny Summers, Satoshi Yagitani. 2009
293 citations recorded by the source corpus.
Subfields: Astronomy and Astrophysics, Geophysics
View Paper: https://www.semanticscholar.org/paper/6901e900b44573345ec726c3c9a5637aa8542599
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Citations in the corpus
- Fine structure of large‐amplitude chorus wave packets (2014, background): “These values are consistent with a possible nonlinear generation mechanism of the fine structure of chorus related to the threshold amplitude for the nonlinear wave growth [Omura et al., 2009;Omura and Nunn, 2011; Kurita et al., 2012; Summers et al., 2013].”
- Theory and observation of electromagnetic ion cyclotron triggered emissions in the magnetosphere (2010, background): “2ps Ws !ð Þ2 " # 1 : ð23Þ The wave equations (21) and (22) take essentially the same forms as the wave equations for a whistler‐mode wave [Omura and Matsumoto, 1982; Omura et al., 2009].”
- Cluster observations of EMIC triggered emissions in association with Pc1 waves near Earth's plasmapause (2010, background): “Omura et al. [2008, 2009] for VLF chorus generation, it is possible for the EMIC triggered emissions to be generated through a nonlinear absolute instability for L‐mode EMIC Figure 2. STAFF‐SC and EFW data from CLUSTER 4 showing the Pc1 waves at ∼ 1.5 Hz and the EMIC triggered emissions rising from”
- An unusual enhancement of low‐frequency plasmaspheric hiss in the outer plasmasphere associated with substorm‐injected electrons (2013, background): “Chorus waves are believed to be excited due to cyclotron resonance with anisotropic energetic electrons (a few keV to ~100 keV) injected from the plasma sheet [Kennel and Petschek, 1966; Anderson and Maeda, 1977; Meredith et al., 2001; Omura et al., 2009].”
- Modeling the evolution of chorus waves into plasmaspheric hiss (2011, background): “…are at present not well understood and remain a topic of intense research [e.g., Nunn, 1971; 1974; Nunn et al., 2009; Trakhtengerts et al., 1996, 2004; Shklyar and Matsumoto, 2009; Bespalov et al., 2010; Lampe et al., 2010; Omura et al., 2008, 2009; Schriver et al., 2010; Santolik et al., 2010].”
- Electron losses from the radiation belts caused by EMIC waves (2014, background): “Although, particularly, chorus waves are known to be highly nonlinear due to their short-duration rising tone frequency structure [e.g., Omura et al., 2009; Santoĺık et al., 2014], it is not yet computationally feasible to simulate chorus waves using nonlinear models over the duration and spatial…”
- Resonant scattering of plasma sheet electrons leading to diffuse auroral precipitation: 2. Evaluation for whistler mode chorus waves (2011, background): “[6] Nonlinear wave growth theories have also been developed to better understand the generation process and wave characteristics of chorus emissions [e.g., Nunn et al., 1997, 2009; Omura et al., 2008, 2009].”
- Three‐dimensional electron radiation belt simulations using the BAS Radiation Belt Model with new diffusion models for chorus, plasmaspheric hiss, and lightning‐generated whistlers (2014, background): “In view of the fact that chorus interactions are highly nonlinear [e.g., Trakhtengerts, 1999; Nunn et al., 1997; Omura et al., 2009], quasi-linear theory is surprisingly good at reproducing the observed variations in electron flux.”