Proceedings of 36th International Cosmic Ray Conference — PoS(ICRC2019) 2019
DOI: 10.22323/1.358.1144
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Modeling the 2017 September 10 Long Duration Gamma Ray Flare

Abstract: to 10 were significant microwave events with revealing multi-wavelength images of the flare environment. The event on September 10 was a large long-duration, gamma-ray flare (LDGRF). The event also produced a Ground Level Enhancement (GLE). Using the constraints from the microwave imaging data from the Expanded Owens Valley Solar Array (EOVSA) we interpret and model the behavior of the energetic-flare protons of September 10 as measured with the Large Area Telescope (LAT) on the Fermi mission. We do this in th… Show more

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Cited by 1 publication
(2 citation statements)
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“…A natural alternative to the CME-shock scenario is represented by the flare-loop model (Ryan & Lee 1991;Mandzhavidze & Ramaty 1992;Chupp & Ryan 2009;Grechnev et al 2018;Ryan & de Nolfo 2018;de Nolfo et al 2019;Ryan et al 2019;de Nolfo et al 2021). If particles are produced and injected on closed field lines, all of them will tend to precipitate on the solar atmosphere after a relatively long residence time associated with particle trapping and second-order Fermi acceleration.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…A natural alternative to the CME-shock scenario is represented by the flare-loop model (Ryan & Lee 1991;Mandzhavidze & Ramaty 1992;Chupp & Ryan 2009;Grechnev et al 2018;Ryan & de Nolfo 2018;de Nolfo et al 2019;Ryan et al 2019;de Nolfo et al 2021). If particles are produced and injected on closed field lines, all of them will tend to precipitate on the solar atmosphere after a relatively long residence time associated with particle trapping and second-order Fermi acceleration.…”
Section: Discussionmentioning
confidence: 99%
“…Despite the significant progress in recent years as a result of the observations of the Fermi Large Area Telescope (LAT; see Ajello et al 2021 and references therein), the involved processes are still controversial. Two main competing scenarios have been proposed to explain the acceleration of the interacting particles responsible for the origin of LDGRFs and their subsequent precipitation into the solar atmosphere: (1) particle trapping with/without continuous acceleration within large (1 R e ) coronal loops, characterized by a delayed onset representing the time required by the ions to exceed the pion production threshold energy (Ryan & Lee 1991;Mandzhavidze & Ramaty 1992;Chupp & Ryan 2009;Grechnev et al 2018;Ryan & de Nolfo 2018;de Nolfo et al 2019;Ryan et al 2019;de Nolfo et al 2021), and (2) coronal mass ejection (CME)-driven shock acceleration, i.e., the dominant mechanism for gradual solar energetic particle (SEP) events measured in situ (Wild et al 1963;Ramaty et al 1987;Cliver et al 1993;Kocharov et al 2015;Pesce-Rollins et al 2015;Plotnikov et al 2017;Gopalswamy et al 2018a;Jin et al 2018;Kahler et al 2018;Kouloumvakos et al 2020). In the latter case, the high-energy photon emission is also referred to as late-phase γ-ray emission (Share et al 2018) or sustained γ-ray emission (Kahler et al 2018).…”
Section: Introductionmentioning
confidence: 99%