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arXiv · 1610.04328

Temporal evolution and spatial distribution of white-light flare kernels in a solar flare

Tomoko Kawate·Takako T. Ishii·Yoshikazu Nakatani·Kiyoshi Ichimoto·Ayumi Asai·Satoshi Morita·Satoshi Masuda
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Abstract

On 2011 September 6, we observed an X2.1-class flare in continuum and H$α$ with a frame rate of about 30~Hz. After processing images of the event by using a speckle-masking image reconstruction, we identified white-light (WL) flare ribbons on opposite sides of the magnetic neutral line. We derive the lightcurve decay times of the WL flare kernels at each resolution element by assuming that the kernels consist of one or two components that decay exponentially, starting from the peak time. As a result, 42% of the pixels have two decay-time components with average decay times of 15.6 and 587 s, whereas the average decay time is 254 s for WL kernels with only one decay-time component. The peak intensities of the shorter decay-time component exhibit good spatial correlation with the WL intensity, whereas the peak intensities of the long decay-time components tend to be larger in the early phase of the flare at the inner part of the flare ribbons, close to the magnetic neutral line. The average intensity of the longer decay-time components is 1.78 times higher than that of the shorter decay-time components. If the shorter decay time is determined by either the chromospheric cooling time or the nonthermal ionization timescale and the longer decay time is attributed to the coronal cooling time, this result suggests that WL sources from both regions appear in 42% of the WL kernels and that WL emission of the coronal origin is sometimes stronger than that of chromospheric origin.

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Tomoko Kawate, Takako T. Ishii, Yoshikazu Nakatani, Kiyoshi Ichimoto, Ayumi Asai, Satoshi Morita, Satoshi Masuda. 2016-10-14. Temporal evolution and spatial distribution of white-light flare kernels in a solar flare. https://doi.org/10.3847/1538-4357%2F833%2F1%2F50

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