Spectral Features of the Solar Transition Region and Chromospheric Lines at Flare Ribbons Observed with IRIS

TL;DR

This study analyzes spectral line features in solar flare ribbons observed with IRIS, revealing how line shifts and reversals vary with flare class and indicating complex chromospheric and transition region dynamics during flares.

Contribution

It provides new insights into the spectral behavior of key lines during flares, especially the optical thickness of Si IV and its relation to flare strength and electron beam heating.

Findings

Redshift velocities decrease with flare class.

Mg II lines show blue-wing enhancements at flare fronts.

Si IV line can become optically thick in strong flares.

Abstract

We report on the spectral features of the Si IV 1402.77 \AA, C II 1334.53 \AA, and Mg II h or k lines, formed in the layers from the transition region to the chromosphere, in three two-ribbon flares (with X-, M-, and C-class) observed with IRIS. All the three lines show significant redshifts within the main flare ribbons, which mainly originate from the chromospheric condensation during the flares. The average redshift velocities of the Si IV line within the main ribbons are 56.6, 25.6, and 10.5 km s$^{-1}$ for the X-, M-, and C-class flares, respectively, which show a decreasing tendency with the flare class. The C II and Mg II lines show a similar tendency but with smaller velocities compared to the Si IV line. Additionally, the Mg II h or k line shows a blue-wing enhancement in the three flares in particular at the flare ribbon fronts, which is supposed to be caused by an upflow in the upper chromosphere due to the heating of the atmosphere. Moreover, the Mg II h or k line exhibits a central reversal at the flare ribbons, but turns to pure emission shortly after 1--4 minutes. Correspondingly, the C II line also shows a central reversal but in a smaller region. However, for the Si IV line, the central reversal is only found in the X-class flare, but not in the other two flares. As usual, the central reversal of these lines can be caused by the opacity effect. This implies that in addition to the optically thick lines (C II and Mg II lines), the Si IV line can become optically thick in a strong flare, which is likely related to the nonthermal electron beam heating.