Formation of Isolated Radio Type II Bursts at Low Frequencies

dc.contributor.authorPohjolainen Silja
dc.contributor.authorTalebpour Sheshvan Nasrin
dc.contributor.organizationfi=Tuorlan observatorio|en=Tuorla Observatory|
dc.contributor.organizationfi=avaruustutkimuslaboratorio|en=Space Research Laboratory|
dc.contributor.organization-code1.2.246.10.2458963.20.47833719389
dc.contributor.organization-code1.2.246.10.2458963.20.90670098848
dc.converis.publication-id58937477
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/58937477
dc.date.accessioned2022-10-28T13:37:52Z
dc.date.available2022-10-28T13:37:52Z
dc.description.abstractThe first appearance of radio type II burst emission at decameter-hectometer (DH) waves typically occurs in connection, and often simultaneously, with other types of radio emissions. As type II bursts are signatures of propagating shock waves that are associated with flares and coronal mass ejections (CMEs), a rich variety of radio emissions can be expected. However, sometimes DH type II bursts appear in the dynamic spectra without other or earlier radio signatures. One explanation for them could be that the flare-CME launch happens on the far side of the Sun, and the emission is observed only when the source gets high enough in the solar atmosphere. In this study we have analysed 26 radio type II bursts that started at DH waves and were well-separated ('isolated') from other radio emission features. These bursts were identified from all DH type II bursts observed in 1998 - 2016, and for 12 events we had observations from at least two different viewing angles with the instruments on board Wind and the Solar Terrestrial Relations Observatory (STEREO) satellites. We found that only 30% of the type II bursts had their source origin on the far side of the Sun, but also that no bursts originated from the central region of the Sun (longitudes E30 - W40). Almost all of the isolated DH type II bursts could be associated with a shock near the CME leading front, and only few were determined to be shocks near the CME flank regions. In this respect our result differs from earlier findings. Our analysis, which included inspection of various CME and radio emission characteristics, suggests that the isolated DH type II bursts could be a special subgroup within DH type II bursts, where the radio emission requires particular coronal conditions to form and to die out.
dc.identifier.eissn1573-093X
dc.identifier.jour-issn0038-0938
dc.identifier.olddbid183227
dc.identifier.oldhandle10024/166321
dc.identifier.urihttps://www.utupub.fi/handle/11111/35515
dc.identifier.urlhttps://link.springer.com/article/10.1007/s11207-021-01828-y
dc.identifier.urnURN:NBN:fi-fe2021093048703
dc.language.isoen
dc.okm.affiliatedauthorPohjolainen, Silja
dc.okm.affiliatedauthorTalebpour Sheshvan, Nasrin
dc.okm.discipline115 Astronomy and space scienceen_GB
dc.okm.discipline115 Avaruustieteet ja tähtitiedefi_FI
dc.okm.internationalcopublicationnot an international co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherSPRINGER
dc.publisher.countryNetherlandsen_GB
dc.publisher.countryAlankomaatfi_FI
dc.publisher.country-codeNL
dc.relation.articlenumberARTN 81
dc.relation.doi10.1007/s11207-021-01828-y
dc.relation.ispartofjournalSolar Physics
dc.relation.volume296
dc.source.identifierhttps://www.utupub.fi/handle/10024/166321
dc.titleFormation of Isolated Radio Type II Bursts at Low Frequencies
dc.year.issued2021

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