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Formation and eruption of filament channel in solar active region 12975: insights from observations and simulations of magnetic field evolution

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dc.contributor.author Mishra, Dinesh
dc.contributor.author Vemareddy, P
dc.contributor.author Kumar, Brajesh
dc.date.accessioned 2026-09-23T05:03:05Z
dc.date.available 2026-09-23T05:03:05Z
dc.date.issued 2026-08-20
dc.identifier.citation The Astrophysical Journal, Vol. 1007, No. 2, 134
dc.identifier.issn 1538-4357
dc.identifier.uri http://hdl.handle.net/2248/9051
dc.description Open Access en_US
dc.description Original content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.
dc.description.abstract We studied the magnetic field evolution of active region (AR) 12975 using a time-dependent magnetofrictional model. This AR produced two consecutive coronal mass ejections associated with M-class flares on 2022 March 28. The AR exhibited a simple bipolar configuration, with new bipolar flux emerging from March 27. These emerging flux regions evolved through shear motions, forming a filament-channel that ultimately erupted on March 28 at 12:00 UT. The simulation, initialized at 12:00 UT on March 26, is driven by electric fields derived from a time-series of photospheric vector-magnetograms. It reproduces the observed coronal evolution, including the gradual development of a sigmoidal, twisted flux rope (FR) over approximately 50 hr. The modeled temporal evolution of magnetic energy and helicity within the computational domain is consistent with the observed injection of both quantities. Furthermore, the ratio of current-carrying to total relative helicity reaches 0.23 at the time of observed eruption; however, the torus-unstable regime is attained when the helicity ratio reaches 0.32, approximately 7 hr after the observed eruption. Notably, the FR forms adjacent to preexisting magnetic fields, and a substantial portion of the coronal structure does not belong to the FR system. Consequently, the derived helicity thresholds vary and deviate from the proposed value of 0.29. While reproducing filament formation with high morphological accuracy, this study underscores the challenges involved in modeling and evaluating the eruptive behavior of different ARs. en_US
dc.language.iso en en_US
dc.publisher American Astronomical Society en_US
dc.relation.uri https://doi.org/10.3847/1538-4357/ae844c
dc.rights © The Author(s) 2026
dc.subject Solar physics en_US
dc.subject Solar photosphere en_US
dc.subject Magnetic fields en_US
dc.subject Solar magnetic fields en_US
dc.subject Solar coronal mass ejections en_US
dc.title Formation and eruption of filament channel in solar active region 12975: insights from observations and simulations of magnetic field evolution en_US
dc.type Article en_US


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