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. 2023 Aug 25;13:13945. doi: 10.1038/s41598-023-40112-w

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© The Author(s) 2023

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.

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Measured radiation patterns in the standard case when scanning to $- 30^{\circ}$ in azimuth, normalized to the peak amplitude in (a), and the gain settings used to excite the array in (b). In (d) the pattern is shown when an additional Taylor taper is applied, and the respective gain settings are shown in (e). In (c) examples of the beam shapes are shown for the transmitter panel using the standard and Taylor taper case. In (f) the scanning gain is shown for all measured scanning angles, normalized to the center beam of each situation.