Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/8139
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dc.contributor.authorRamesh, R-
dc.contributor.authorKathiravan, C-
dc.date.accessioned2023-02-03T04:48:41Z-
dc.date.available2023-02-03T04:48:41Z-
dc.date.issued2022-11-20-
dc.identifier.citationThe Astrophysical Journal, Vol. 940, No. 1, 80en_US
dc.identifier.issn1538-4357-
dc.identifier.urihttp://hdl.handle.net/2248/8139-
dc.descriptionOpen Accessen_US
dc.descriptionOriginal content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.-
dc.description.abstractUsing temporal observations of circular polarized harmonic plasma emission from a split-band type II solar radio burst at 80 MHz, we separately estimated the coronal magnetic field strengths (B) associated with the lower (L) and upper (U) frequency bands of the burst. The corresponding Stokes I and V data were obtained with the polarimeter operating at the above frequency in the Gauribidanur observatory. The burst was associated with a flare/coronal mass ejection on the solar disk. Simultaneous spectral observations with the spectrograph there in the frequency range 80–35 MHz helped to establish that the observed polarized emission was from the harmonic component of the burst. The B values corresponding to the polarized emission from the L and U bands at 80 MHz are BL ≈ 1.2 G and BU ≈ 2.4 G, respectively. The different values of B for the observed harmonic emission at the same frequency (80 MHz) from the two bands imply unambiguously that the corresponding fundamental emission at 40 MHz must have originated at different spatial locations. Two-dimensional radio imaging observations of the burst with the radioheliograph in the same observatory at 80 MHz indicate the same. As comparatively higher B is expected behind a propagating shock due to compression as well as the corresponding coronal regions being closer to the Sun, our results indicate that the sources of L- and U-band emission should be located ahead of and behind the associated coronal shock, respectively. These are useful to understand the pre- and postshock corona as well as locations of electron acceleration in a propagating shock.en_US
dc.language.isoenen_US
dc.publisherAmerican Astronomical Societyen_US
dc.relation.urihttps://doi.org/10.3847/1538-4357/ac9c65-
dc.rights© 2022. The Author(s).-
dc.subjectSolar coronaen_US
dc.subjectThe Sunen_US
dc.subjectRadio burstsen_US
dc.subjectPolarimetryen_US
dc.subjectSolar coronal mass ejectionsen_US
dc.subjectSolar flaresen_US
dc.subjectSolar magnetic fieldsen_US
dc.titlePolarization Observations of a Split-band Type II Radio Burst from the Solar Coronaen_US
dc.typeArticleen_US
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