Evolution of the magnetic field distribution of active regions

被引:8
作者
Dacie, S. [1 ]
Demoulin, P. [2 ]
van Driel-Gesztelyi, L. [1 ,2 ,3 ]
Long, D. M. [1 ]
Baker, D. [1 ]
Janvier, M. [4 ]
Yardley, S. L. [1 ]
Perez-Suarez, D. [1 ]
机构
[1] Univ Coll London, Mullard Space Sci Lab, Holmbury RH5 6NT, Surrey, England
[2] CNRS, UMR 8109, LESIA, Observ Paris, F-92195 Meudon, France
[3] Hungarian Acad Sci, Konkoly Observ, H-1121 Budapest, Hungary
[4] Univ Paris Saclay, CNRS, Univ Paris Sud, Inst Astrophys Spatiale,UMR8617, Batiment 121, F-91405 Orsay, France
关键词
magnetic fields; Sun: photosphere; Sun: evolution; sunspots; methods: statistical; methods: analytical; PROBABILITY DENSITY-ESTIMATION; FLUX TUBES; EMERGENCE; FLARES; TOPOLOGY; DYNAMICS; DECAY; LAW;
D O I
10.1051/0004-6361/201628948
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Aims. Although the temporal evolution of active regions (ARs) is relatively well understood, the processes involved continue to be the subject of investigation. We study how the magnetic field of a series of ARs evolves with time to better characterise how ARs emerge and disperse. Methods. We examined the temporal variation in the magnetic field distribution of 37 emerging ARs. A kernel density estimation plot of the field distribution was created on a log-log scale for each AR at each time step. We found that the central portion of the distribution is typically linear, and its slope was used to characterise the evolution of the magnetic field. Results. The slopes were seen to evolve with time, becoming less steep as the fragmented emerging flux coalesces. The slopes reached a maximum value of similar to-1.5 just before the time of maximum flux before becoming steeper during the decay phase towards the quiet-Sun value of similar to-3. This behaviour differs significantly from a classical diffusion model, which produces a slope of -1. These results suggest that simple classical diffusion is not responsible for the observed changes in field distribution, but that other processes play a significant role in flux dispersion. Conclusions. We propose that the steep negative slope seen during the late-decay phase is due to magnetic flux reprocessing by (super) granular convective cells.
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页数:11
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