2018
DOI: 10.1029/2018ja025179
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Kinetic‐Scale Ion Flux Fluctuations Behind the Quasi‐Parallel and Quasi‐Perpendicular Bow Shock

Abstract: Properties of kinetic‐scale plasma turbulence are examined observationally with the help of Spektr‐R measurements in the Earth's magnetosheath. The statistics covers 6 years of ion flux measurements during years 2011–2017 and includes a few dozens of the magnetosheath crossings with total duration of 250 hr. Several types of Fourier spectra are distinguished in the magnetosheath according to a spectral shape at the scales of transition from magnetohydrodynamic to kinetic regimes. Spectral indices and occurrenc… Show more

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Cited by 20 publications
(29 citation statements)
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“…Moreover, the spectral scaling at sub-ion scales flattens from the bow shock to the flank and the magnetopause. Similar results are obtained for the ion-flux spectra in the dayside magnetosheath (Rakhmanova et al 2018b(Rakhmanova et al , 2018a.…”
Section: Introductionsupporting
confidence: 85%
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“…Moreover, the spectral scaling at sub-ion scales flattens from the bow shock to the flank and the magnetopause. Similar results are obtained for the ion-flux spectra in the dayside magnetosheath (Rakhmanova et al 2018b(Rakhmanova et al , 2018a.…”
Section: Introductionsupporting
confidence: 85%
“…Various wave modes/ instabilities introduced immediately after the bow shock (e.g., Schwartz et al 1996) may be responsible for these phenomena. Rakhmanova et al (2018a) show that "bump"-type ion-flux spectra (i.e., peaked at 0.25-0.35 Hz) are more likely observed near the bow shock rather than near the magnetopause, which leads to spectral flattening at MHD scales and spectral steepening at sub-ion scales. Sahraoui et al (2006) argue that mirror-mode structures are more likely responsible for the "bumps" in magnetic field and plasma spectra with the peak at ∼0.1 Hz.…”
Section: From the Bow Shock To The Magnetopausementioning
confidence: 90%
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“…This range is usually defined by achange of the PSD steepness (relative to the inertial range). For PSDs of bulk V sw and thermal velocity, V th , the spectral index steepens to values between −2 and −4 (Šafránková et al 2016), whereas for N the slope first flattens (Unti et al 1973;Chen et al 2013b;Šafránková et al 2015) and then decreases to avalue of −2.8 (Alexandrova et al 2009;Chen et al 2012b;Šafránková et al 2015;Riazantseva et al 2016;Rakhmanova et al 2018). In the range between the ion and electron scales, magnetic field fluctuations typically exhibit aspectral scaling similar to that of the density…”
Section: Introductionmentioning
confidence: 99%