Spatio-temporal structure of storm-time chorus
By O. Santolík, Donald A. Gurnett, J. Pickett, M. Parrot, N. Cornilleau-Wehrlin. 2003
397 citations recorded by the source corpus.
Subfields: Astronomy and Astrophysics, Geophysics
View Paper: https://www.semanticscholar.org/paper/b819c11c28ff3298e9f4af7d4699c1e71c0d008b
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Citations in the corpus
- Resonant scattering of plasma sheet electrons by whistler‐mode chorus: Contribution to diffuse auroral precipitation (2008, background): “[10] During geomagnetically disturbed conditions upperband chorus wave amplitudes can vary over a large range from 10 pT to above 100 pT [e.g., Meredith et al., 2001; Santolik et al., 2003], in the present study we have chosen a slightly high but reasonably intermediate wave amplitude.”
- Evaluation of quasi-linear diffusion coefficients for whistler mode waves in a plasma with arbitrary density ratio (2005, methodology): “To perform numerical integrations, the code described here relied on Romberg’s method, adapted from the implementation of Press et al. [1992] .”
- Modeling the evolution of chorus waves into plasmaspheric hiss (2011, background): “…2008] is shown in Figure 1b. Individual chorus elements are usually narrowband, meaning that each chorus element consists of a central frequency that varies with time (df/dt ≠ 0), and a small bandwidth centered on this central frequency on the order of ∼10 Hz [e.g., Santolik et al., 2003].”
- Discovery of very large amplitude whistler‐mode waves in Earth's radiation belts (2008, methodology): “Acceleration of electrons by low amplitude whistler-mode ‘chorus’ waves is currently accepted to be an important process in the outer belt [Summers et al., 1998; Roth et al., 1999; Summers and Ma, 2000; Meredith et al., 2001; Horne and Thorne, 2003; Horne et al., 2005; Albert and Young, 2005].”
- Timescale for MeV electron microburst loss during geomagnetic storms (2005, methodology): “The properties of chorus have been described in previous studies [e.g., Tsurutani and Smith, 1977; Meredith et al., 2003; Santolik et al., 2003].”
- Resonant scattering of plasma sheet electrons leading to diffuse auroral precipitation: 2. Evaluation for whistler mode chorus waves (2011, background): “…are usually confined to within 20° of the magnetic field for both bands, predominantly parallel or quasi‐parallel to the ambient magnetic field [Burton and Holzer, 1974; Goldstein and Tsurutani, 1984; Santolík et al., 2003], in agreement with theoretical predictions [Kennel and Thorne, 1967].”
- THEMIS observations of long‐lived regions of large‐amplitude whistler waves in the inner magnetosphere (2008, background): “[3] Observations by Santolk et al. [2003] of >30 mV/m parallel-propagating whistler-mode waves, and by Cattell et al. [2008] of >250 mV/m oblique whistlers, suggest a new paradigm for acceleration by whistler waves.”
- THEMIS analysis of observed equatorial electron distributions responsible for the chorus excitation (2010, background): “…fce) and upper band (0.5 fce < f < 0.7 fce) with a gap at 0.5 fce, where fce is the equatorial electron cyclotron frequency [Burtis and Helliwell, 1969; Tsurutani and Smith, 1977; Hayakawa et al., 1984; Koons and Roeder, 1990; Sazhin and Hayakawa, 1992; Santolík et al., 2003; Bell et al., 2009].”
- Constructing the global distribution of chorus wave intensity using measurements of electrons by the POES satellites and waves by the Van Allen Probes (2013, background): “[2] Magnetospheric whistler-mode chorus waves are intense coherent electromagnetic emissions exhibiting discrete rising or falling tones in the magnetosphere [Burtis and Helliwell, 1969; Tsurutani and Smith, 1974; Santolik et al., 2003].”
- Earth's Van Allen Radiation Belts: From Discovery to the Van Allen Probes Era (2019, background): “However, realistic chorus wave packets are found to exhibit rising or falling tones with subpacket structures (e.g., Li et al., 2012; Santolík et al., 2003, 2014), and most of them have short wave packet length (<10 wave periods; X. Zhang, Thorne, et al., 2018).”
- Nonlinear mechanisms of lower-band and upper-band VLF chorus emissions in the magnetosphere (2009, methodology): “…fact that the source location of chorus elements is indeed confirmed by recent spacecraft278 observations to be close to the magnetic equator [e.g., Santolik et al., 2003].279 At the equator the inhomogeneity of the magnetic field is zero, and the second term on280 the right-hand side of(10)…”