Imaging spectroscopy of a spectral bump in a type II radio burst

dc.contributor.authorZhang Peijin
dc.contributor.authorMorosan Diana E.
dc.contributor.authorZucca Pietro
dc.contributor.authorNormo Sanna
dc.contributor.authorDabrowski Bartosz
dc.contributor.authorKrankowski Andrzej
dc.contributor.authorVocks Christian
dc.contributor.organizationfi=avaruustutkimuslaboratorio|en=Space Research Laboratory|
dc.contributor.organization-code1.2.246.10.2458963.20.47833719389
dc.converis.publication-id393461699
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/393461699
dc.date.accessioned2025-08-28T01:42:52Z
dc.date.available2025-08-28T01:42:52Z
dc.description.abstract<p>Context. Observations of solar, type II radio bursts provide a unique opportunity to analyze the nonthermal electrons accelerated by coronal shocks and diagnose the plasma density distribution in the corona. However, there are very few high-frequency resolution interferometric observations of type II radio bursts that are capable of tracking these electrons. <br></p><p>Aims. Recently, more spatially resolved high-resolution observations of type II radio bursts have been recorded with the Low-Frequency Array (LOFAR). Using these observations, we aim to track the location of a type II radio burst that experienced a sudden spectral bump. <br></p><p>Methods. We present the first radio imaging observations of a type II burst with a spectral bump. We measured the variation in source location and frequency drift of the burst and deducted the density distribution along its propagation direction. <br></p><p>Results. We have identified a type II burst that experiences a sudden spectral bump in its frequency-time profile. The overall frequency drift rate is 0.06 MHz s−1, and this corresponds to an estimated speed of 295 km s−1. The projected velocity of the radio source obtained from imaging is 380 km s−1 toward the east. At the spectral bump, a deviation in the source locations of the type II split bands is observed. The band separation increases significantly in the north–south direction. <br></p><p>Conclusions. The spectral bump shows an 8 MHz deviation at 60 MHz, which corresponds to a 25% decrease in the plasma density. The estimated crossing distance during the spectrum bump was 29 mm, suggesting that this density variation occurs in a confined area. This indicates that the shock most likely encountered the upper extent of a coronal hole. © The Authors 2024.</p>
dc.identifier.eissn1543-5474
dc.identifier.jour-issn0004-6361
dc.identifier.olddbid207940
dc.identifier.oldhandle10024/190967
dc.identifier.urihttps://www.utupub.fi/handle/11111/57337
dc.identifier.urlhttps://doi.org/10.1051/0004-6361/202449365
dc.identifier.urnURN:NBN:fi-fe2025082791826
dc.language.isoen
dc.okm.affiliatedauthorMorosan, Diana
dc.okm.affiliatedauthorNormo, Sanna
dc.okm.discipline115 Astronomy and space scienceen_GB
dc.okm.discipline115 Avaruustieteet ja tähtitiedefi_FI
dc.okm.internationalcopublicationinternational co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherEDP Sciences
dc.publisher.countryFranceen_GB
dc.publisher.countryRanskafi_FI
dc.publisher.country-codeFR
dc.relation.articlenumberL22
dc.relation.doi10.1051/0004-6361/202449365
dc.relation.ispartofjournalAstronomy and Astrophysics
dc.relation.volume684
dc.source.identifierhttps://www.utupub.fi/handle/10024/190967
dc.titleImaging spectroscopy of a spectral bump in a type II radio burst
dc.year.issued2024

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