Table 2.
Overview of the observations.
Instrument | λ [Å]a | Line/feature | log T [K]d | Atmospheric regimee | |
---|---|---|---|---|---|
SDO | HMI | 6173 | Magnetogramb | – | Photosphere |
AIA | 1600 | Continuumc | <3.6 | Upper photosphere / T-minf | |
2796.9 | Mg II k1r | 3.6 | T-min / lower chromosphere | ||
2796.6 | Mg II k2r | 3.8 | Middle chromosphere | ||
IRIS | 2796.4 | Mg II k3 | 3.9 | Upper chromosphere | |
1335.7 | C II | 4.6 | Low transition region | ||
1393.8 | Si IV | 4.9 | Transition region |
Notes.
The AIA 1600 Å images are acquired in a roughly 50 Å wide wavelength band. For lines observed with IRIS the wavelength of the respective features of the Mg II k line or the rest wavelength of C II and Si IV are given (see Sect. 2.2.1).
In active regions HMI can also provide the full vector of the magnetic field. We use the line-of-sight component of the magnetic field from HMI.
This 1600 Å band contains also the C IV doublet at 1548 Å and 1550 Å. Except for small patches of strongly enhanced emission around 105 K this band does not show transition region structures on the disc (e.g. compare panels b and d in Fig. 2).
The formation temperatures for the 1600 Å continuum and the Mg II k line features are taken from (Vernazza et al. 1981), the values for C II and Si IV are taken from (Peter 2006).
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