2020
DOI: 10.1007/s11207-020-01686-0
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Estimate of Plasma Temperatures Across a CME-Driven Shock from a Comparison Between EUV and Radio Data

Abstract: In this work, we analyze the evolution of an EUV wave front associated with a solar eruption that occurred on 30 October 2014, with the aim of investigating, through differential emission measure (DEM) analysis, the physical properties of the plasma compressed and heated by the accompanying shock wave. The EUV wave was observed by the Atmospheric Imaging Assembly (AIA) onboard the Solar Dynamics Observatory (SDO) and was accompanied by the detection of a metric Type II burst observed by ground-based radio spec… Show more

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Cited by 15 publications
(14 citation statements)
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“…Although this is typically estimated using radio data by examining the difference in frequency between the fundamental and harmonic frequencies of the shock, the type II emission observed here corresponds to the leading edge of the CME-driven shock rather than the laterally driven global wave shock, and could therefore provide an inaccurate estimate of the shock strength. Instead, the density compression ratio can be estimated by examining the change in EUV intensity and/or DEM (see Kozarev et al 2011;Ma et al 2011;Muhr et al 2011;Zhukov 2011;Frassati et al 2019;Long et al 2019;Frassati et al 2020). The EUV density compression ratio (X) was estimated here using both the intensity ratio approach of Zhukov (2011) and the DEM ratio approach of Frassati et al (2019).…”
Section: Plasma Diagnosticsmentioning
confidence: 99%
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“…Although this is typically estimated using radio data by examining the difference in frequency between the fundamental and harmonic frequencies of the shock, the type II emission observed here corresponds to the leading edge of the CME-driven shock rather than the laterally driven global wave shock, and could therefore provide an inaccurate estimate of the shock strength. Instead, the density compression ratio can be estimated by examining the change in EUV intensity and/or DEM (see Kozarev et al 2011;Ma et al 2011;Muhr et al 2011;Zhukov 2011;Frassati et al 2019;Long et al 2019;Frassati et al 2020). The EUV density compression ratio (X) was estimated here using both the intensity ratio approach of Zhukov (2011) and the DEM ratio approach of Frassati et al (2019).…”
Section: Plasma Diagnosticsmentioning
confidence: 99%
“…While initially characterized using either wave or pseudo-wave interpretations (see Warmuth 2015), recent work (see Long et al 2017b;Downs et al 2021) has made it increasingly evident that these features can best be interpreted as large-amplitude waves/shocks. The multi-wavelength observations provided by SDO have also enabled plasma diagnostics of these perturbations, showing an adiabatic increase in both temperature and density associated with their passage through the solar corona (Vanninathan et al 2015;Long et al 2019;Frassati et al 2020). However, in each case, these results have underlined the very weak nature of these shocks, finding Mach numbers only slightly greater than 1 (e.g., Long et al 2015;Frassati et al 2020).…”
Section: Introductionmentioning
confidence: 99%
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“…Type II bursts and herringbones represent signatures of electron beams accelerated at the CME shock (e.g. Mann & Klassen 2005;Morosan et al 2019a;Frassati et al 2020). Type IV radio bursts are defined by a continuum emission at decimetric and metric wavelengths in dynamic spectra that can show stationary or moving sources, or both, that are emitted by various emission mechanisms (e.g.…”
Section: Introductionmentioning
confidence: 99%
“…Type II bursts and herringbones represent signatures of electron beams accelerated at the CME shock (e.g. Mann & Klassen 2005;Morosan et al 2019a;Frassati et al 2020). Type IV radio bursts are defined by a continuum emission at decimetric and metric wavelengths in dynamic spectra that can show stationary or moving sources, or both, that are emitted by various emis-sion mechanisms (e.g.…”
Section: Introductionmentioning
confidence: 99%