Heating manifestations at the onset of the 29 June 2012 flare

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Analysis of GOES data for the SOL2012-06-29T04:09 flare, class C4.6, shows a thermal character of the energy release for several minutes before the impulsive stage. Plasma heating to temperatures above 10 MK leads to the appearance of plasma jets along open field lines and in large loops. This work examines the relationship between the heated plasma and the flare structure and its dynamics, using observations in the X-ray, extreme ultraviolet (EUV), and radio-wave ranges. Particular attention is drawn to the detection of narrow-band fine temporal structures of radio emission before and after the impulsive stage of the flare in dynamic spectra. In the initial stage, broadband pulses in the decimeter range are observed which can be associated with the formation of thermal fronts in the jets. A series of super-bright drifting bursts in the centimeter range occurs after the end of the impulsive energy release in the flare kernel. Using data from the Siberian Solar Radio Telescope (5.7 GHz), we managed to localize the position of the source of the fine structure of drifting bursts at the remote footpoint of the large-scale flare loop.

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Analysis of GOES data for the SOL2012-06-29T04:09 flare, class C4.6, shows a thermal character of the energy release for several minutes before the impulsive stage. Plasma heating to temperatures above 10 MK leads to the appearance of plasma jets along open field lines and in large loops. This work examines the relationship between the heated plasma and the flare structure and its dynamics, using observations in the X-ray, extreme ultraviolet (EUV), and radio-wave ranges. Particular attention is drawn to the detection of narrow-band fine temporal structures of radio emission before and after the impulsive stage of the flare in dynamic spectra. In the initial stage, broadband pulses in the decimeter range are observed which can be associated with the formation of thermal fronts in the jets. A series of super-bright drifting bursts in the centimeter range occurs after the end of the impulsive energy release in the flare kernel. Using data from the Siberian Solar Radio Telescope (5.7 GHz), we managed to localize the position of the source of the fine structure of drifting bursts at the remote footpoint of the large-scale flare loop.

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view Abstract Citations (30) References (43) Co-Reads Similar Papers Volume Content Graphics Metrics Export Citation NASA/ADS Energy Propagation into a Flare Kernel during a Solar Flare Melrose, D. B. Abstract A model for energy propagation into the energy release site is formulated in terms of Alfvenic fronts where stored magnetic energy is partially converted into an energy flux. It is found that, irrespective of the model's details, the energy released in a flare kernel cannot be simply the energy stored within the energy release site. Energy must flow into the energy release site, predominantly along the mean magnetic field, from at least the entire coronal portion of the flaring flux tube. Some energy can also flow into the corona from below the photosphere during a flare, but this is unlikely to be important in the impulsive phase of the flare. When the energy release turns on in a flare kernel, the system responds by creating two fronts that propagate away from the energy release site at the Alfven speed. Part of the initial current flowing through the energy release site is deflected at the front so that it flows around the energy release site. Publication: The Astrophysical Journal Pub Date: March 1992 DOI: 10.1086/171092 Bibcode: 1992ApJ...387..403M Keywords: Energy Transfer; Magnetohydrodynamic Waves; Solar Corona; Solar Flares; Wave Propagation; Energy Dissipation; Photosphere; Rotating Plasmas; Solar Magnetic Field; Solar Physics; MAGNETOHYDRODYNAMICS: MHD; SUN: FLARES full text sources ADS |

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