4.7 Article

ELECTRON ENERGY PARTITION IN THE ABOVE-THE-LOOPTOP SOLAR HARD X-RAY SOURCES

Journal

ASTROPHYSICAL JOURNAL
Volume 799, Issue 2, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.1088/0004-637X/799/2/129

Keywords

acceleration of particles; Sun: flares; Sun: X-rays; gamma rays

Funding

  1. NASA [NAS 5-98033]
  2. NASA at UC Berkeley [NNX08AO83G]

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Solar flares produce non-thermal electrons with energies up to tens of MeVs. To understand the origin of energetic electrons, coronal hardX-ray (HXR) sources, in particular above-the-looptop sources, have been studied extensively. However, it still remains unclear how energies are partitioned between thermal and non-thermal electrons within the above-the-looptop source. Here we show that the kappa distribution, when compared to conventional spectral models, can better characterize the above-the-looptop HXRs (greater than or similar to 15 keV) observed in four different cases. The widely used conventional model (i.e., the combined thermal plus power-law distribution) can also fit the data, but it returns unreasonable parameter values due to a non-physical sharp lower-energy cutoff E-c. In two cases, extreme-ultraviolet data were available from SDO/AIA and the kappa distribution was still consistent with the analysis of differential emission measure. Based on the kappa distribution model, we found that the 2012 July 19 flare showed the largest non-thermal fraction of electron energies about 50%, suggesting equipartition of energies. Considering the results of particle-in-cell simulations, as well as density estimates of the four cases studied, we propose a scenario in which electron acceleration is achieved primarily by collisionless magnetic reconnection, but the electron energy partition in the above-the-looptop source depends on the source density. In low-density above-the-looptop regions (few times 10(9) cm(-3)), the enhanced non-thermal tail can remain and a prominent HXR source is created, whereas in higher-densities (> 10(10) cm(-3)), the non-thermal tail is suppressed or thermalized by Coulomb collisions.

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