Abstract

Aims. We study the structure and dynamics of three Ellerman bombs (EBs) observed in an evolving active region.Methods. The active region NOAA 11271 was observed with the Vacuum Tower Telescope at Observatorio del Teide/Tenerife on August 18, 2011. We used the two-dimensional Triple Etalon SOlar Spectrometer (TESOS) to obtain time sequences of the active region and of EBs in Hα at a cadence of 15 s. Simultaneously, we obtained full Stokes profiles with the Tenerife Infrared Polarimeter (TIP II) in the two magnetically sensitive Fe i infrared lines (IR) at 1.56 μ , scanning spatial sections of the area with cadences of 28−46 s. The Hα data were reconstructed with speckle methods to study the evolution of the atmospheric stratification. Two methods were used to extract magnetic field information from the IR Stokes profiles: 1) fitting of the (Q,U,V ) profiles by Gaussians; and 2) applying the Milne-Eddington approximation, assuming two separate magnetic structures in the resolution element and fitting by trial and error some profiles from the EB areas. Data from SDO-HMI and -AIA were also used. We performed two-dimensional (2D) non-LTE radiative transfer calculations of Hα in parameterised models of EBs.Results. The three EBs studied in detail occurred in a complex active region near sunspots. They were very bright with a factor of 1.5–2.8 brighter than the nearby area. They lived for 1/2 h and longer. They were related to broadband faculae, but the latter were not the brightest features in the field of view. The EBs occurred in magnetic field configurations with opposite polarity close together. One EB was located at the outskirts of a penumbra of a complex sunspot and showed repeated “flaring” in SDO-AIA data. Another was close to a strong field patch and moved into this during the end of its lifetime. The third EB showed clear changes of field structure during the time it was observed. We obtained from the 2D modelling that heating and increase in Hα opacity are likely to occur at heights of 300–800 km. Line shifts and asymmetries can well be reproduced by velocities at these heights and also at much larger heights.Conclusions. The three EBs occurred at sites with magnetic fields of opposite polarity, which were likely the cause of the Hα brightening upon reconnection.

Highlights

  • Evolving active regions (ARs) of the Sun, when observed in hydrogen Balmer lines, show conspicuous, short-duration brightenings, known as the Ellerman bombs (EBs, Ellerman 1917)

  • We show in Sect. 4.3.4 that the Stokes profiles require at least two magnetic fields with different strengths and orientations within the spatial resolution element in many cases within and near EBs

  • EB 1 had a field of mainly positive polarity, but we show in Sect. 4.3.4 that it contains a negative polarity field

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Summary

Introduction

Evolving active regions (ARs) of the Sun, when observed in hydrogen Balmer lines, show conspicuous, short-duration brightenings, known as the Ellerman bombs (EBs, Ellerman 1917). Matsumoto et al (2008) carried out observations in Ca ii H and of 6302 Stokes (I, V) with HINODE/SOT at a cadence of 6 min and took simultaneous Hα filtergrams with the Hida solar telescope at a cadence of 7 min They found magnetic dipoles close to an EB and a substructure in EBs that is seen in Ca ii H as a core and a halo. Using Hα filtergrams and vector magnetograms from Hida observatory, Watanabe et al (2008) found EBs in areas of undulatory magnetic fields of emerging flux regions They suggested three different field topologies in which EBs are triggered: 1) at the foot point of converging magnetic fields of opposite polarity; 2) above BPs; and 3) in QSLs. A photometric analysis of EBs was performed by Berlicki et al (2010).

Observations
Image reconstruction and time sequences
Correction for parasitic light
Infrared lines from TIP II
Ellerman bomb positions in AR
Maps of Ellerman bombs and near surroundings
Flows of granular pattern
Hαwing contrasts
Evolution of intensities and magnetic fields
Modelling procedure
Contrasts from models
Line shifts and asymmetries
Conclusions
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