Coronal Conditions for the Occurrence of Type II Radio Bursts

dc.bibliographicCitation.firstPage99
dc.bibliographicCitation.issue2
dc.bibliographicCitation.journalTitleThe astrophysical journal : an international review of spectroscopy and astronomical physics : Part 1eng
dc.bibliographicCitation.volume913
dc.contributor.authorKouloumvakos, Athanasios
dc.contributor.authorRouillard, Alexis
dc.contributor.authorWarmuth, Alexander
dc.contributor.authorMagdalenic, Jasmina
dc.contributor.authorJebaraj, Immanuel. C.
dc.contributor.authorMann, Gottfried
dc.contributor.authorVainio, Rami
dc.contributor.authorMonstein, Christian
dc.date.accessioned2023-04-19T04:39:11Z
dc.date.available2023-04-19T04:39:11Z
dc.date.issued2021
dc.description.abstractType II radio bursts are generally observed in association with flare-generated or coronal-mass-ejection-driven shock waves. The exact shock and coronal conditions necessary for the production of type II radio emission are still under debate. Shock waves are important for the acceleration of electrons necessary for the generation of the radio emission. Additionally, the shock geometry and closed field line topology, e.g., quasi-perpendicular shock regions or shocks interacting with streamers, play an important role for the production of the emission. In this study we perform a 3D reconstruction and modeling of a shock wave observed during the 2014 November 5 solar event. We determine the spatial and temporal evolution of the shock properties and examine the conditions responsible for the generation and evolution of type II radio emission. Our results suggest that the formation and evolution of a strong, supercritical, quasi-perpendicular shock wave interacting with a coronal streamer were responsible for producing type II radio emission. We find that the shock wave is subcritical before and supercritical after the start of the type II emission. The shock geometry is mostly quasi-perpendicular throughout the event. Our analysis shows that the radio emission is produced in regions where the supercritical shock develops with an oblique to quasi-perpendicular geometry.eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/12009
dc.identifier.urihttp://dx.doi.org/10.34657/11042
dc.language.isoeng
dc.publisherLondon : Institute of Physics Publ.
dc.relation.doihttps://doi.org/10.3847/1538-4357/abf435
dc.relation.essn1538-4357
dc.relation.issn0004-637X
dc.rights.licenseCC BY 4.0 Unported
dc.rights.urihttps://creativecommons.org/licenses/by/4.0
dc.subject.ddc520
dc.subject.otherSolar radio emissioneng
dc.subject.otherSolar coronal mass ejectionseng
dc.subject.otherSolar coronal mass ejection shockseng
dc.titleCoronal Conditions for the Occurrence of Type II Radio Burstseng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccess
wgl.contributorAIP
wgl.subjectPhysikger
wgl.typeZeitschriftenartikelger
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