2022
DOI: 10.1117/1.jatis.8.1.011017
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Computational electromagnetics for the SKA-Low prototype station AAVS2

Abstract: We summarize the activities conducted since 2019 in the numerical electromagnetic analysis of one prototype station of the SKA-Low telescope. Working closely with the SKA Observatory, two teams based in Australia and Italy have collaborated effectively in modeling and analyzing AAVS2, which is the most recent prototype of an SKA-Low station installed in Western Australia. A comprehensive overview of the main electromagnetic parameters at element and array level obtained with two different commercial solvers is… Show more

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Cited by 29 publications
(24 citation statements)
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“…For instance, the full-wave analysis of 256 SKALA4.1 antennas by means of the multilevel fast multipole method along with the method of moment technique requires on the order of days for each frequency point on a multicore workstation. 13 Alternative techniques to accelerate the solution of Maxwell equations in the context of SKA1-Low were proposed in Ref. 14.…”
Section: Introductionmentioning
confidence: 99%
“…For instance, the full-wave analysis of 256 SKALA4.1 antennas by means of the multilevel fast multipole method along with the method of moment technique requires on the order of days for each frequency point on a multicore workstation. 13 Alternative techniques to accelerate the solution of Maxwell equations in the context of SKA1-Low were proposed in Ref. 14.…”
Section: Introductionmentioning
confidence: 99%
“…The Galactic plane has a more pronounced morphological difference, particularly at 55 MHz for the XX polarization and close to the horizon (panels C, left side). This discrepancy may be due to mutual coupling from the antennas, 5,15 which is more prominent near the horizon and is not accounted for in our simulations. We also note that our simulated images do not include the station uv coverage and this can also cause slight differences between observed and simulated images, although a more quantitative comparison is left for the future.…”
Section: Observations and Data Processingmentioning
confidence: 85%
“…We rather fixed the absolute flux density scale by multiplying each flux density and noise measurement of our analysis (see Sections 3.1,4.1, 4.2) by the primary beam response corresponding to the Sun position in the snapshot observation used for calibration, normalized to zenith. We assumed that all the antennas have the same primary beam, the average embedded element pattern (hereafter EEP) 5,15 .…”
Section: Observations and Data Processingmentioning
confidence: 99%
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