Design of Wideband Vivaldi Antenna Array

Author(s):  
Chang Liu ◽  
Chenjiang Guo ◽  
Haobin Zhang
IEEE Access ◽  
2020 ◽  
Vol 8 ◽  
pp. 118299-118304 ◽  
Author(s):  
Won-Woo Lee ◽  
In-June Hwang ◽  
Beakcheol Jang

2013 ◽  
Vol 380-384 ◽  
pp. 3465-3468
Author(s):  
Hai Bo Tang ◽  
Xiao Zhong Shui

Firstly in this paper,an antipodal Vivaldi antenna is designed.The bandwidth is from 6GHz to 18GHz. The simulated results show good electric performance and the voltage standing wave ratio is less than 2 in the whole bandwidth.Secondly depending on this unit,this paper designs two kinds of arrays and estimates their radiation characteristics,respectively.The one array is a 1×8 array and the another array is a X-cross structure array with four elements.


2016 ◽  
Vol 2016 ◽  
pp. 1-11 ◽  
Author(s):  
Zengrui Li ◽  
Xiaole Kang ◽  
Jianxun Su ◽  
Qingxin Guo ◽  
Yaoqing (Lamar) Yang ◽  
...  

The characteristics of a novel antipodal Vivaldi antenna array mounted on a dielectric cone are presented. By employing antipodal Vivaldi antenna element, the antenna array shows ultrawide bandwidth and end-fire radiation characteristics. Our simulations show that the cone curvature has an obvious influence on the performance of the conformal antenna, in terms of both the bandwidth and the radiation patterns. The thickness and permittivity of the dielectric cone have an effect on the bandwidth of the conformal antenna. Measurement results of both single antenna and conformal antenna array show a good agreement with the simulated results. The measured conformal antenna can achieve a −10 dBS11with bandwidth of 2.2–12 GHz and demonstrate a typical end-fire radiation beam. These findings provide useful guidelines and insights for the design of wideband end-fire antennas mounted on a dielectric cone.


2018 ◽  
Vol 17 (5) ◽  
pp. 776-779 ◽  
Author(s):  
Shuangshuang Zhu ◽  
Haiwen Liu ◽  
Zhijiao Chen ◽  
Pin Wen

2019 ◽  
Vol 27 (1) ◽  
pp. 92-98 ◽  
Author(s):  
M. Biancheri-Astier ◽  
A. Diet ◽  
Y. le Bihan ◽  
M. Grzeskowiak

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