Abstract

Context. The dynamical nature of fine structures in prominences remains an open issue, including rotating flows in tornado prominences. While the Atmospheric Imaging Assembly imager aboard the Solar Dynamics Observatory allowed us to follow the global structure of a tornado-like prominence for five hours, the Interface Region Imaging Spectrograph, and the Multichannel Subtractive Double Pass spectrograph permitted to obtain plasma diagnostics of its fine structures. Aims. We aim to address two questions. Firstly, is the observed plasma rotation conceptually acceptable in a flux rope magnetic support configuration with dips? Secondly, how is the plasma density distributed in the tornado-like prominence? Methods. We calculated line-of-sight velocities and non-thermal line widths using Gaussian fitting for Mg II lines and the bisector method for Hα line. We determined the electron density from Mg II line integrated intensities and profile fitting methods using 1D non-LTE radiative transfer theory models. Results. The global structure of the prominence observed in Hα, and Mg II h, and k line fits with a magnetic field structure configuration with dips. Coherent Doppler shifts in redshifted and blueshifted areas observed in both lines were detected along rapidly-changing vertical and horizontal structures. However, the tornado at the top of the prominence consists of multiple fine threads with opposite flows, suggesting counter-streaming flows rather than rotation. Surprisingly we found that the electron density at the top of the prominence could be larger (1011 cm−3) than in the inner part of the prominence. Conclusions. We suggest that the tornado is in a formation state with cooling of hot plasma in a first phase, and following that, a phase of leakage of the formed blobs with large transverse flows of material along long loops extended away from the UV prominence top. The existence of such long magnetic field lines on both sides of the prominence would stop the tornado-like prominence from really turning around its axis.

Highlights

  • Solar prominences are dense and cool plasma structures (104 K) embedded in the hot solar corona (106 K)

  • A simultaneous multi-instrumental observation campaign comprising of Interface Region Imaging Spectrograph (IRIS), Hinode, the Multi subtractive Double pass spectrograph (MSDP) spectrograph (operating at the Meudon solar tower (MST)), Solar Dynamics Observatory (SDO)/Atmospheric Imaging Assembly (AIA) and other observatories focussed on a solar prominence which had manifested on the south-west (S51) solar limb on the 19th April 2018

  • Prominences observed in this line look completely different from how they are seen in Hα but similar to what is seen in IRIS Slit Jaw Imager (SJI) 2796

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Summary

Introduction

Solar prominences are dense and cool plasma structures (104 K) embedded in the hot solar corona (106 K). With spectrographs (such as the Extreme-ultraviolet Imaging Spectrometer (EIS - Culhane et al (2007)) aboard Hinode, the Interface Region Imaging Spectrograph (De Pontieu et al 2014, IRIS) or from ground-based observatories) such motions were observed as blueshift on one side, and redshift on the other side of vertical columns in prominences This suggests twisted magnetic structures or tornadoes (Orozco Suárez et al 2012; Su et al 2014; Levens et al 2016; Yang et al 2018). A simultaneous multi-instrumental observation campaign comprising of IRIS, Hinode, the MSDP spectrograph (operating at the Meudon solar tower (MST)), SDO/AIA and other observatories focussed on a solar prominence which had manifested on the south-west (S51) solar limb on the 19th April 2018 This prominence corresponds to one anchorage-footpoint of a long east-west filament visible in Hα on 16 April, with dark equidistant bushes along its axis (data in BASS2000.com). Krzysztof Barczynski et al.: Spectro-imagery of an active tornado-like prominence: formation and evolution

Instruments
Evolution of the large-scale prominence in different temperatures
Tornado-prominence dynamics
Mg ii : Wavelength calibration method
Mg ii: Gaussian fitting method
Mg ii: Quantile method
Co-alignment IRIS and MSDP data
Hα Dopplershifts
Mask definition for Mg ii prominence
Magnetic field configuration
Plasma characteristics from observations and theory
Mg ii and Hα profiles
Interpretation with a 1D radiative transfer code
Correlation between Mg ii and Hα lines and emission measure
Observed and synthesized profiles
Electron density and optical thickness
Discussion and conclusion
Full Text
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