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Polarization Observations of a Split-band Type II Radio Burst from the Solar Corona

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dc.contributor.author Ramesh, R
dc.contributor.author Kathiravan, C
dc.date.accessioned 2023-02-03T04:48:41Z
dc.date.available 2023-02-03T04:48:41Z
dc.date.issued 2022-11-20
dc.identifier.citation The Astrophysical Journal, Vol. 940, No. 1, 80 en_US
dc.identifier.issn 1538-4357
dc.identifier.uri http://hdl.handle.net/2248/8139
dc.description Open Access en_US
dc.description Original 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.abstract Using 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.iso en en_US
dc.publisher American Astronomical Society en_US
dc.relation.uri https://doi.org/10.3847/1538-4357/ac9c65
dc.rights © 2022. The Author(s).
dc.subject Solar corona en_US
dc.subject The Sun en_US
dc.subject Radio bursts en_US
dc.subject Polarimetry en_US
dc.subject Solar coronal mass ejections en_US
dc.subject Solar flares en_US
dc.subject Solar magnetic fields en_US
dc.title Polarization Observations of a Split-band Type II Radio Burst from the Solar Corona en_US
dc.type Article en_US


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