Interface Region Imaging Spectrograph (IRIS) Observations of the Fractal Dimension in the Solar Atmosphere

preprint2022arXivOpen access

Abstract

While previous work explored the fractality and self-organized criticality (SOC) of flares and nanoflares in wavelengths emitted in the solar corona (such as in hard X-rays, soft X-rays, and EUV wavelenghts), we focus here on impulsive phenomena in the photosphere and transition region, as observed with the {\sl Interface Region Imaging Spectrograph (IRIS)} in the temperature range of Te≈104−106T_e \approx 10^4-10^6 K. We find the following fractal dimensions (in increasing order): DA=1.21±0.07D_A=1.21 \pm 0.07 for photospheric granulation, DA=1.29±0.15D_A=1.29 \pm 0.15 for plages in the transition region, DA=1.54±0.16D_A=1.54 \pm 0.16 for sunspots in the transition region, DA=1.59±0.08D_A=1.59 \pm 0.08 for magnetograms in active regions, DA=1.56±0.08D_A=1.56 \pm 0.08 for EUV nanoflares, DA=1.76±0.14D_A=1.76 \pm 0.14 for large solar flares, and up to DA=1.89±0.05D_A=1.89 \pm 0.05 for the largest X-class flares. We interpret low values of the fractal dimension ($1.0 \lapprox D_A \lapprox 1.5$) in terms of sparse curvi-linear flow patterns, while high values of the fractal dimension ($1.5 \lapprox D_A \lapprox 2.0$) indicate near space-filling transport processes, such as chromospheric evaporation. Phenomena in the solar transition region appear to be consistent with SOC models, based on their size distributions of fractal areas AA and (radiative) energies EE, which show power law slopes of αAobs=2.51±0.21α_A^{obs}=2.51 \pm 0.21 (with αAtheo=2.33α_A^{theo}=2.33 predicted), and αEobs=2.03±0.18α_E^{obs}=2.03 \pm 0.18 (with αEtheo=1.80α_E^{theo}=1.80 predicted).

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