TY - JOUR
T1 - Magnetic structure of an activated filament in a flaring active region
AU - Sasso, C.
AU - Lagg, A.
AU - Solanki, S. K.
N1 - Funding Information:
We thank Aad Van Ballegooijgen for reading a draft of this paper and generously providing suggestions. We thank the referee, Arturo López Ariste, for useful suggestions and comments. C.S. thanks the IMPRS on Physical Processes in the Solar System and Beyond for the opportunity to carry out the research presented in this paper. This work was supported by the ASI-INAF contract ASI N. I/013/12/0, Work Package 1310 – Operazioni Scientifiche. This work has been partially supported by the WCU grant No. R31-10016 funded by the Korean Ministry of Education, Science and Technology.
PY - 2014/1
Y1 - 2014/1
N2 - Aims. While the magnetic field in quiescent prominences has been widely investigated, less is known about the field in activated prominences. We report observational results on the magnetic field structure of an activated filament in a flaring active region. In particular, we studied its magnetic structure and line-of-sight flows during its early activated phase, shortly before it displayed signs of rotation. Methods. We inverted the Stokes profiles of the chromospheric He i 10 830 Å triplet and the photospheric Si i 10 827 Å line observed in this filament by the Vacuum Tower Telescope on Tenerife. Using these inversion results, we present and interpret the first maps of the velocity and magnetic field obtained in an activated filament, both in the photosphere and the chromosphere. Results. Up to five different magnetic components are found in the chromospheric layers of the filament, while outside the filament a single component is sufficient to reproduce the observations. Magnetic components displaying an upflow are preferentially located towards the centre of the filament, while the downflows are concentrated along its periphery. Moreover, the upflowing gas is associated with an opposite-polarity magnetic configuration with respect to the photosphere, while the downflowing gas is associated with a same-polarity configuration. Conclusions. The activated filament has a very complex structure. Nonetheless, it is compatible with a flux rope, albeit a distorted one, in the normal configuration. The observations are best explained by a rising flux rope in which part of the filament material is still stably stored (upflowing material, rising with the field), while the rest is no longer stably stored and flows down along the field lines.
AB - Aims. While the magnetic field in quiescent prominences has been widely investigated, less is known about the field in activated prominences. We report observational results on the magnetic field structure of an activated filament in a flaring active region. In particular, we studied its magnetic structure and line-of-sight flows during its early activated phase, shortly before it displayed signs of rotation. Methods. We inverted the Stokes profiles of the chromospheric He i 10 830 Å triplet and the photospheric Si i 10 827 Å line observed in this filament by the Vacuum Tower Telescope on Tenerife. Using these inversion results, we present and interpret the first maps of the velocity and magnetic field obtained in an activated filament, both in the photosphere and the chromosphere. Results. Up to five different magnetic components are found in the chromospheric layers of the filament, while outside the filament a single component is sufficient to reproduce the observations. Magnetic components displaying an upflow are preferentially located towards the centre of the filament, while the downflows are concentrated along its periphery. Moreover, the upflowing gas is associated with an opposite-polarity magnetic configuration with respect to the photosphere, while the downflowing gas is associated with a same-polarity configuration. Conclusions. The activated filament has a very complex structure. Nonetheless, it is compatible with a flux rope, albeit a distorted one, in the normal configuration. The observations are best explained by a rising flux rope in which part of the filament material is still stably stored (upflowing material, rising with the field), while the rest is no longer stably stored and flows down along the field lines.
KW - Sun: chromosphere
KW - Sun: filaments, prominences
KW - Sun: infrared
KW - Sun: magnetic fields
UR - http://www.scopus.com/inward/record.url?scp=84892413132&partnerID=8YFLogxK
U2 - 10.1051/0004-6361/201322481
DO - 10.1051/0004-6361/201322481
M3 - Article
AN - SCOPUS:84892413132
SN - 0004-6361
VL - 561
JO - Astronomy and Astrophysics
JF - Astronomy and Astrophysics
M1 - A98
ER -