Generation of OAM Radio Waves Using Circular Vivaldi Antenna Array

This paper gives a feasible and simple solution of generating OAM-carrying radio beams. Eight Vivaldi antenna elements connect sequentially and fold into a hollow cylinder. The circular Vivaldi antenna array is fed with unit amplitude but with a successive phase difference from element to element. B...

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Main Authors: Changjiang Deng, Wenhua Chen, Zhijun Zhang, Yue Li, Zhenghe Feng
Format: Article
Language:English
Published: Hindawi Limited 2013-01-01
Series:International Journal of Antennas and Propagation
Online Access:http://dx.doi.org/10.1155/2013/847859
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spelling doaj-301827c782a34863a84830d8144a166f2020-11-24T23:28:18ZengHindawi LimitedInternational Journal of Antennas and Propagation1687-58691687-58772013-01-01201310.1155/2013/847859847859Generation of OAM Radio Waves Using Circular Vivaldi Antenna ArrayChangjiang Deng0Wenhua Chen1Zhijun Zhang2Yue Li3Zhenghe Feng4State Key Laboratory of Microwave and Digital Communication, Tsinghua University, Beijing 100084, ChinaState Key Laboratory of Microwave and Digital Communication, Tsinghua University, Beijing 100084, ChinaState Key Laboratory of Microwave and Digital Communication, Tsinghua University, Beijing 100084, ChinaState Key Laboratory of Microwave and Digital Communication, Tsinghua University, Beijing 100084, ChinaState Key Laboratory of Microwave and Digital Communication, Tsinghua University, Beijing 100084, ChinaThis paper gives a feasible and simple solution of generating OAM-carrying radio beams. Eight Vivaldi antenna elements connect sequentially and fold into a hollow cylinder. The circular Vivaldi antenna array is fed with unit amplitude but with a successive phase difference from element to element. By changing the phase difference at the steps of 0, ±45°, ±90°, ±135°, and 180°, the OAM radio beam can be generated with mode numbers 0, ±1, ±2, ±3, and 4. Simulations show that the OAM states of ±2 and ±3 are the same as the traditional states, while the OAM states of 0, ±1, and 4 differ at the boresight. This phenomenon can be explained by the radiation pattern difference between Vivaldi antenna and tripole antenna. A solution of distinguishing OAM states is also proposed. The mode number of OAM can be distinguished with only 2 receivers.http://dx.doi.org/10.1155/2013/847859
collection DOAJ
language English
format Article
sources DOAJ
author Changjiang Deng
Wenhua Chen
Zhijun Zhang
Yue Li
Zhenghe Feng
spellingShingle Changjiang Deng
Wenhua Chen
Zhijun Zhang
Yue Li
Zhenghe Feng
Generation of OAM Radio Waves Using Circular Vivaldi Antenna Array
International Journal of Antennas and Propagation
author_facet Changjiang Deng
Wenhua Chen
Zhijun Zhang
Yue Li
Zhenghe Feng
author_sort Changjiang Deng
title Generation of OAM Radio Waves Using Circular Vivaldi Antenna Array
title_short Generation of OAM Radio Waves Using Circular Vivaldi Antenna Array
title_full Generation of OAM Radio Waves Using Circular Vivaldi Antenna Array
title_fullStr Generation of OAM Radio Waves Using Circular Vivaldi Antenna Array
title_full_unstemmed Generation of OAM Radio Waves Using Circular Vivaldi Antenna Array
title_sort generation of oam radio waves using circular vivaldi antenna array
publisher Hindawi Limited
series International Journal of Antennas and Propagation
issn 1687-5869
1687-5877
publishDate 2013-01-01
description This paper gives a feasible and simple solution of generating OAM-carrying radio beams. Eight Vivaldi antenna elements connect sequentially and fold into a hollow cylinder. The circular Vivaldi antenna array is fed with unit amplitude but with a successive phase difference from element to element. By changing the phase difference at the steps of 0, ±45°, ±90°, ±135°, and 180°, the OAM radio beam can be generated with mode numbers 0, ±1, ±2, ±3, and 4. Simulations show that the OAM states of ±2 and ±3 are the same as the traditional states, while the OAM states of 0, ±1, and 4 differ at the boresight. This phenomenon can be explained by the radiation pattern difference between Vivaldi antenna and tripole antenna. A solution of distinguishing OAM states is also proposed. The mode number of OAM can be distinguished with only 2 receivers.
url http://dx.doi.org/10.1155/2013/847859
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