Publication:
SIMULATIONS of LATERAL TRANSPORT and DROPOUT STRUCTURE of ENERGETIC PARTICLES from IMPULSIVE SOLAR FLARES

dc.contributor.authorP. Tooprakaien_US
dc.contributor.authorA. Seripienlerten_US
dc.contributor.authorD. Ruffoloen_US
dc.contributor.authorP. Chuychaien_US
dc.contributor.authorW. H. Matthaeusen_US
dc.contributor.otherChulalongkorn Universityen_US
dc.contributor.otherSouth Carolina Commission on Higher Educationen_US
dc.contributor.otherMahidol Universityen_US
dc.contributor.otherRajamangala University of Technology Thanyaburi (RMUTT)en_US
dc.contributor.otherBurapha Universityen_US
dc.contributor.otherBartol Research Instituteen_US
dc.date.accessioned2018-12-11T02:43:50Z
dc.date.accessioned2019-03-14T08:04:39Z
dc.date.available2018-12-11T02:43:50Z
dc.date.available2019-03-14T08:04:39Z
dc.date.issued2016-11-10en_US
dc.description.abstract© 2016. The American Astronomical Society. All rights reserved. We simulate trajectories of energetic particles from impulsive solar flares for 2D+slab models of magnetic turbulence in spherical geometry to study dropout features, i.e., sharp, repeated changes in the particle density. Among random-phase realizations of two-dimensional (2D) turbulence, a spherical harmonic expansion can generate homogeneous turbulence over a sphere, but a 2D fast Fourier transform (FFT) locally mapped onto the lateral coordinates in the region of interest is much faster computationally, and we show that the results are qualitatively similar. We then use the 2D FFT field as input to a 2D MHD simulation, which dynamically generates realistic features of turbulence such as coherent structures. The magnetic field lines and particles spread non-diffusively (ballistically) to a patchy distribution reaching up to 25° from the injection longitude and latitude at r ∼ 1 au. This dropout pattern in field line trajectories has sharper features in the case of the more realistic 2D MHD model, in better qualitative agreement with observations. The initial dropout pattern in particle trajectories is relatively insensitive to particle energy, though the energy affects the pattern's evolution with time. We make predictions for future observations of solar particles near the Sun (e.g., at 0.25 au), for which we expect a sharp pulse of outgoing particles along the dropout pattern, followed by backscattering that first remains close to the dropout pattern and later exhibits cross-field transport to a distribution that is more diffusive, yet mostly contained within the dropout pattern found at greater distances.en_US
dc.identifier.citationAstrophysical Journal. Vol.831, No.2 (2016)en_US
dc.identifier.doi10.3847/0004-637X/831/2/195en_US
dc.identifier.issn15384357en_US
dc.identifier.issn0004637Xen_US
dc.identifier.other2-s2.0-84994481858en_US
dc.identifier.urihttps://repository.li.mahidol.ac.th/handle/20.500.14594/43589
dc.rightsMahidol Universityen_US
dc.rights.holderSCOPUSen_US
dc.source.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84994481858&origin=inwarden_US
dc.subjectEarth and Planetary Sciencesen_US
dc.titleSIMULATIONS of LATERAL TRANSPORT and DROPOUT STRUCTURE of ENERGETIC PARTICLES from IMPULSIVE SOLAR FLARESen_US
dc.typeArticleen_US
dspace.entity.typePublication
mu.datasource.scopushttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84994481858&origin=inwarden_US

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