A Hot Cusp-Shaped Confined Solar Flare
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(Complete draft of No. 371) |
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|name = Nugget | |name = Nugget | ||
|number = 370 | |number = 370 | ||
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|first_author = Aaron Hernandez-Perez | |first_author = Aaron Hernandez-Perez | ||
|second_author = | |second_author = | ||
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rare observations of a <i>confined</i> flare that exhibited an | rare observations of a <i>confined</i> flare that exhibited an | ||
apparent cusp with a temperature distribution distinctly different | apparent cusp with a temperature distribution distinctly different | ||
- | from those reported in literature, | + | from those reported in literature, exhibiting an increasing |
temperature with increasing height even in the absence of an | temperature with increasing height even in the absence of an | ||
eruption. | eruption. | ||
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The flare SOL2014-01-13T21:51 appeared in the low corona at the location | The flare SOL2014-01-13T21:51 appeared in the low corona at the location | ||
- | of nonthermal precursor activity. | + | of substantial nonthermal precursor activity. |
- | + | Particle acceleration related to magnetic reconnection, | |
- | + | subsequent plasma heating and chromospheric | |
- | evaporation, revealed cusp-shaped flare loops extending | + | evaporation, revealed cusp-shaped flare loops extending almost 70 Mm |
- | + | into the corona (Figure 1). | |
[[File:371f1.png|500px|thumb|center|'''Figure 1''': | [[File:371f1.png|500px|thumb|center|'''Figure 1''': | ||
- | Composite of AIA 1600 Â (red) + 304 (blue) + 131 | + | Composite of AIA 1600 Â (red) + 304 Â (blue) + 131 Â (green) images |
showing the (E)UV flare emission during the impulsive phase. The | showing the (E)UV flare emission during the impulsive phase. The | ||
- | 131 emission clearly outlines an overlying system of cusp-shaped | + | 131 Â emission clearly outlines an overlying system of cusp-shaped |
loops toward solar west | loops toward solar west | ||
]] | ]] | ||
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distribution spectral index δ, the cutoff energy, | distribution spectral index δ, the cutoff energy, | ||
E<sub>C</sub>, as well as the chi-squared of the fitting, | E<sub>C</sub>, as well as the chi-squared of the fitting, | ||
- | & | + | Χ<sup>2</sup>, are all listed in the figure legend. |
]] | ]] | ||
Revision as of 18:32, 19 February 2020
Nugget | |
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Number: | 370 |
1st Author: | Aaron Hernandez-Perez |
2nd Author: | |
Published: | 24 February 2020 |
Next Nugget: | The flaring photosphere |
Previous Nugget: | The Temporal and Spatial Extension of Gamma-ray Emission from the Sun |
List all |
Contents |
Introduction
A growing cusp-shaped flare arcade is a typical feature in the standard model of eruptive flares, and is regarded as a signature of magnetic reconnection taking place at progressively larger coronal heights. This feature resulted from 2D approximations to the process, while an earlier Nugget described a generalization to 3D. As reconnection occurs at successively larger heights in the solar corona, the outer flare loops have systematically higher temperatures than the previously reconnected ones, located underneath. We report (Ref. 1 rare observations of a confined flare that exhibited an apparent cusp with a temperature distribution distinctly different from those reported in literature, exhibiting an increasing temperature with increasing height even in the absence of an eruption.
An Atypical Flare Loop
The flare SOL2014-01-13T21:51 appeared in the low corona at the location of substantial nonthermal precursor activity. Particle acceleration related to magnetic reconnection, subsequent plasma heating and chromospheric evaporation, revealed cusp-shaped flare loops extending almost 70 Mm into the corona (Figure 1).
After the impulsive phase, RHESSI X-ray emission, of a partly nonthermal nature, originated from the cusp-shaped structure. This indicates continued particle acceleration during the decay phase (Figure 2). Prolonged hot emission was further observed, consistent with ongoing energy release in the apparent cusp (Figure 3(b)).
Conclusion
Given the observational characteristics, the cusp-shaped appearance of the flare was most probably related to a kinked shape of the magnetic field (Figure 3(a)). The extended enhanced SXR and EUV emission during the late phase provides evidence of a weak process of ongoing energy release. This can also explain the increasing temperature distribution with height observed during the decay phase (Figure 3(b)).
References
[1] "A Hot Cusp-shaped Confined Solar Flare"
RHESSI Nugget Date | 24 February 2020 + |
RHESSI Nugget First Author | Aaron Hernandez-Perez + |
RHESSI Nugget Index | 370 + |