The magnetic topology of the inverse Evershed flow
The magnetic topology of the inverse Evershed flow
复制标题
逆Evershed流的磁拓扑
DOI:
10.1051/0004-6361/202142585
复制
发表时间:
2022
影响因子:
6.5
通讯作者:
Hu, Q.
中科院分区:
文献类型:
--
作者:
Prasad, A.;Ranganathan, M.;Beck, C.;Choudhary, D. P.;Hu, Q.
ContextThe inverse Evershed flow (IEF) is a mass motion towards sunspots at chromospheric heights.AimsWe combined high-resolution observations of NOAA 12418 from the Dunn Solar Telescope and vector magnetic field measurements from the Helioseismic and Magnetic Imager (HMI) to determine the driver of the IEF.MethodsWe derived chromospheric line-of-sight (LOS) velocities from spectra of Hαand Ca II IR. The HMI data were used in a non-force-free magnetic field extrapolation to track closed field lines near the sunspot in the active region. We determined their length and height, located their inner and outer foot points, and derived flow velocities along them.ResultsThe magnetic field lines related to the IEF reach on average a height of 3 megameter (Mm) over a length of 13 Mm. The inner (outer) foot points are located at 1.2 (1.9) sunspot radii. The average field strength difference ΔBbetween inner and outer foot points is +400 G. The temperature difference ΔTis anti-correlated with ΔBwith an average value of −100 K. The pressure difference Δpis dominated by ΔBand is primarily positive with a driving force towards the inner foot points of 1.7 kPa on average. The velocities predicted from Δpreproduce the LOS velocities of 2–10 km s−1with a square-root dependence.ConclusionsWe find that the IEF is driven along magnetic field lines connecting network elements with the outer penumbra by a gas pressure difference that results from a difference in field strength as predicted by the classical siphon flow scenario.