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On the Use of Ridge Gap Waveguide Technology for the Design of Transverse Stub Resonant Antenna Arrays

This paper presents some considerations on the design of a novel antenna consisting of the combination of a transverse stubs (TS) array excited by Ridge Gap Waveguides (RGWs), as well as a discussion of the experimental results obtained from a prototype that was manufactured and measured. A combinat...

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Autores principales: Benavides-Vazquez, Javier, Vazquez-Roy, Jose-Luis, Rajo-Iglesias, Eva
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8512434/
https://www.ncbi.nlm.nih.gov/pubmed/34640910
http://dx.doi.org/10.3390/s21196590
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author Benavides-Vazquez, Javier
Vazquez-Roy, Jose-Luis
Rajo-Iglesias, Eva
author_facet Benavides-Vazquez, Javier
Vazquez-Roy, Jose-Luis
Rajo-Iglesias, Eva
author_sort Benavides-Vazquez, Javier
collection PubMed
description This paper presents some considerations on the design of a novel antenna consisting of the combination of a transverse stubs (TS) array excited by Ridge Gap Waveguides (RGWs), as well as a discussion of the experimental results obtained from a prototype that was manufactured and measured. A combination of Continuous Transverse Stubs (CTSs) is used as the starting point. Subsequently, the CTSs are modified to include some metallic blockers that split each CTS into a combination (array) of shorter TSs. This is performed in order to excite each individual TS column using a different RGW; thus, ensuring a close to uniform field distribution in the transverse plane of the TS arrays. Hence, the directivity of the antenna is increased. As a series-feed configuration is considered, the antenna keeps a resonant behaviour, having a narrow-band response. A Corporate Feeding Network (CFN) using the aforementioned RGW technology placed in the same layer as the rest of the antenna is included in the design. The radiating area of the antenna is, finally, [Formula: see text] with a simulated peak gain of 26.2 dBi and a Side Lobe Level (SLL) below −13 dB. A prototype is manufactured and tested. The simulated and measured radiation patterns maintain similar shapes to those of the simulations, with very similar angular widths in both main planes, although the frequency corresponding to the highest directivity changes to 31.8 GHz. A matching bandwidth of 517 MHz and a gain of 24.5 is, finally, achieved at that frequency.
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spelling pubmed-85124342021-10-14 On the Use of Ridge Gap Waveguide Technology for the Design of Transverse Stub Resonant Antenna Arrays Benavides-Vazquez, Javier Vazquez-Roy, Jose-Luis Rajo-Iglesias, Eva Sensors (Basel) Article This paper presents some considerations on the design of a novel antenna consisting of the combination of a transverse stubs (TS) array excited by Ridge Gap Waveguides (RGWs), as well as a discussion of the experimental results obtained from a prototype that was manufactured and measured. A combination of Continuous Transverse Stubs (CTSs) is used as the starting point. Subsequently, the CTSs are modified to include some metallic blockers that split each CTS into a combination (array) of shorter TSs. This is performed in order to excite each individual TS column using a different RGW; thus, ensuring a close to uniform field distribution in the transverse plane of the TS arrays. Hence, the directivity of the antenna is increased. As a series-feed configuration is considered, the antenna keeps a resonant behaviour, having a narrow-band response. A Corporate Feeding Network (CFN) using the aforementioned RGW technology placed in the same layer as the rest of the antenna is included in the design. The radiating area of the antenna is, finally, [Formula: see text] with a simulated peak gain of 26.2 dBi and a Side Lobe Level (SLL) below −13 dB. A prototype is manufactured and tested. The simulated and measured radiation patterns maintain similar shapes to those of the simulations, with very similar angular widths in both main planes, although the frequency corresponding to the highest directivity changes to 31.8 GHz. A matching bandwidth of 517 MHz and a gain of 24.5 is, finally, achieved at that frequency. MDPI 2021-10-02 /pmc/articles/PMC8512434/ /pubmed/34640910 http://dx.doi.org/10.3390/s21196590 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Benavides-Vazquez, Javier
Vazquez-Roy, Jose-Luis
Rajo-Iglesias, Eva
On the Use of Ridge Gap Waveguide Technology for the Design of Transverse Stub Resonant Antenna Arrays
title On the Use of Ridge Gap Waveguide Technology for the Design of Transverse Stub Resonant Antenna Arrays
title_full On the Use of Ridge Gap Waveguide Technology for the Design of Transverse Stub Resonant Antenna Arrays
title_fullStr On the Use of Ridge Gap Waveguide Technology for the Design of Transverse Stub Resonant Antenna Arrays
title_full_unstemmed On the Use of Ridge Gap Waveguide Technology for the Design of Transverse Stub Resonant Antenna Arrays
title_short On the Use of Ridge Gap Waveguide Technology for the Design of Transverse Stub Resonant Antenna Arrays
title_sort on the use of ridge gap waveguide technology for the design of transverse stub resonant antenna arrays
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8512434/
https://www.ncbi.nlm.nih.gov/pubmed/34640910
http://dx.doi.org/10.3390/s21196590
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