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Solar Radio Spectro-polarimeter (50–500 MHz). I. Design, Development, and Characterization of a Cross-polarized, Log-periodic Dipole Antenna

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dc.contributor.author Kumari, Anshu
dc.contributor.author Gireesh, G. V. S
dc.contributor.author Kathiravan, C
dc.contributor.author Mugundhan, V
dc.contributor.author Barve, Indrajit V
dc.contributor.author Ramesh, R
dc.contributor.author Monstein, C
dc.date.accessioned 2024-01-10T05:30:23Z
dc.date.available 2024-01-10T05:30:23Z
dc.date.issued 2023-12-01
dc.identifier.citation The Astrophysical Journal, Vol. 958, No. 2, 181 en_US
dc.identifier.issn 1538-4357
dc.identifier.uri http://hdl.handle.net/2248/8330
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 The Zeeman effect has been routinely used to image and quantify the solar photospheric magnetic field (B). Such a direct measuring technique is not yet available for the corona (Lin et al. 2004). Since almost all transient nonthermal radio emissions from the corona are either partially or fully circularly polarized, observing their polarization signatures over broad frequency ranges would be of help to estimate B as a function of heliocentric height. This article aims to describe the design and development of a Cross-polarized Log-Periodic Dipole Antenna (CLPDA), an integral part of a radio spectro-polarimeter, which works in the 50–500 MHz frequency-range and to explain the tests that were carried out to characterize it. The above frequency range corresponds to a heliocentric height range ≈1.03 < r < 2.5 Re (Re = photospheric radius), wherein the numerous coronal nonthermal transients associated with space-weather effects are observed to originate. The CLPDA is used to determine the strength and sense of polarization of the received radio signal. The uncertainty involved in the determination depends on the polarization-isolation (PI) between the two orthogonal components of a CLPDA. Some of the recent advancements made in the antenna design concepts at high frequencies (∼GHz) were adopted to reduce the PI at low frequencies (∼MHz). Throughout the above frequency range, the CLPDA has a gain, return loss, and PI of ≈6.6 dBi, −10 dB, and −27 dB, respectively. The average PI of the CLPDA varies from −30 to −24 dB over an azimuthal angle range 0° to ±45° within which the observations are performed regularly. 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/acff58
dc.rights © 2023. The Author(s)
dc.subject Solar radio emission en_US
dc.subject Solar radio telescopes en_US
dc.subject Radio spectroscopy en_US
dc.subject Spectropolarimetry en_US
dc.subject Solar-terrestrial interactions en_US
dc.subject Solar magnetic fields en_US
dc.subject Solar corona en_US
dc.subject Active solar corona en_US
dc.title Solar Radio Spectro-polarimeter (50–500 MHz). I. Design, Development, and Characterization of a Cross-polarized, Log-periodic Dipole Antenna en_US
dc.type Article en_US


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