4.7 Article

Probing the Puzzle of Behind-the-limb γ-Ray Flares: Data-driven Simulations of Magnetic Connectivity and CME-driven Shock Evolution

Journal

ASTROPHYSICAL JOURNAL
Volume 867, Issue 2, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.3847/1538-4357/aae1fd

Keywords

magnetohydrodynamics (MHD); methods: numerical; Sun: corona; Sun: coronal mass ejections (CMEs); Sun: flares; Sun: X-rays, gamma rays

Funding

  1. NASA's SDO/AIA [NNG04EA00C]
  2. NASA HGI [NNX15AR15G, NNX16AF78G, NNX14AJ49G]
  3. NSF [AGS 1322543]
  4. NASA [NNX16AL12G, NNX17AI17G, NNX17AK25G]
  5. NSF AGS [1322543]

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Recent detections of high-energy gamma-rays from behind-the-limb (BTL) solar flares by the Fermi Gamma-ray Space Telescope pose a puzzle and challenge on the particle acceleration and transport mechanisms. In such events, the gamma-ray emission region is located away from the BTL flare site by up to tens of degrees in heliographic longitude. It is thus hypothesized that particles are accelerated at the shock driven by the coronal mass ejection (CME) and then travel from the shock downstream back to the front side of the Sun to produce the observed gamma-rays. To test this scenario, we performed data-driven, global magnetohydrodynamics simulations of the CME associated with a well-observed BTL flare on 2014 September 1. We found that part of the CME-driven shock develops magnetic connectivity with the gamma-ray emission region, facilitating transport of particles back to the Sun. Moreover, the observed increase in gamma-ray flux is temporally correlated with (1) the increase of the shock compression ratio and (2) the presence of a quasi-perpendicular shock over the area that is magnetically connected to the gamma-ray emitting region, both conditions favoring the diffusive shock acceleration (DSA) of particles. These results support the above hypothesis and can help resolve another puzzle, i.e., long-duration (up to 20 hr) gamma-rays flares. We suggest that, in addition to DSA, stochastic acceleration by plasma turbulence may also play a role, especially in the shock downstream region and during the early stage when the shock Alfven Mach number is small.

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