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June 21, 2023

Electron acceleration efficiency during the impulsive phase of a solar flare: X-ray and microwave observations

Left: Clean RHESSI X-ray images using Detectors \#3 and \#6 for the 20 second interval centered on 15:58~UT, with three regions of interest identified. The color-scale image represents thermal (10–12 keV) emission. The blue dashed lines are the contours at 20, 70, and 90% of the peak 50–100 keV non-thermal emission. The region of interest labeled ROI-0 is defined by the solid blue contour at the 50% level of the 50–100 keV image. Regions of interest ROI-1 and ROI-2 are depicted by solid black and magenta boundary lines, respectively. Right: Thermal plasma density map, also showing ROI-1 and ROI-2. This was constructed by applying a regularized differential emission measure algorithm (Hannah & Kontar, 2012) to SDO/AIA data for the event in question, assuming the same line-of-sight distance of 8′′ used by Fleishman et al, 2022. Credit: Kontar et al, 2023
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Left: Clean RHESSI X-ray images using Detectors \#3 and \#6 for the 20 second interval centered on 15:58~UT, with three regions of interest identified. The color-scale image represents thermal (10–12 keV) emission. The blue dashed lines are the contours at 20, 70, and 90% of the peak 50–100 keV non-thermal emission. The region of interest labeled ROI-0 is defined by the solid blue contour at the 50% level of the 50–100 keV image. Regions of interest ROI-1 and ROI-2 are depicted by solid black and magenta boundary lines, respectively. Right: Thermal plasma density map, also showing ROI-1 and ROI-2. This was constructed by applying a regularized differential emission measure algorithm (Hannah & Kontar, 2012) to SDO/AIA data for the event in question, assuming the same line-of-sight distance of 8′′ used by Fleishman et al, 2022. Credit: Kontar et al, 2023

Solar flares are known to be prolific electron accelerators, yet identifying the mechanism(s) for such efficient electron acceleration in magnetic reconnection events at the sun (and similar astrophysical settings) presents a . Accelerated electrons with energies above ∼20 keV are revealed by hard X-ray (HXR) bremsstrahlung emission, while accelerated electrons with even higher energies usually manifest themselves through radio gyrosynchrotron emission.

Of considerable interest is the nature of the process that accelerates particles to high energies and the ratios of the number densities (cm−3) of nonthermal and thermal electrons (nnth and nth, respectively) to the total number density of background electrons in acceleration region.

Recently Eduard Kontar and colleagues combined RHESSI HXR observations of a well-observed with contemporaneous EUV observations from the Solar Dynamics Observatory Atmospheric Imaging Assembly in order to better constrain both the total number of accelerated electrons and the all-important ratio (nnth/np) in the 10 September 2017 solar flare that revealed clear evidence for a reconnection current sheet located above the flare loop-top.

The results indicate that the ratio of nonthermal electrons to ambient electrons in ROI-1 at a time near the peak of the X-ray emission is nnth/np ≃ 0.01–0.02. The findings are published in The Astrophysical Journal Letters.

Intriguingly, the microwave spectrum analysis by using 2" , which are smaller than EOVSA beam resolution of (45−5)" for the (2−18) GHz range, gives approximately 100 times larger fraction of accelerated in the same region of flare.

More information: Eduard P. Kontar et al, The Efficiency of Electron Acceleration during the Impulsive Phase of a Solar Flare, The Astrophysical Journal Letters (2023).

Journal information: Astrophysical Journal Letters

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