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 |