Abstract

A composite cavity-based antenna is proposed and presented in this work. Three kinds of modes of the composite structure are involved to obtain a wide bandwidth: the ${\mathrm {TE}}_{11 {\scriptstyle {}^{\scriptstyle 1}}\hspace {-0.224em}/\hspace {-0.112em}{\scriptstyle 2} }$ cavity mode of a cylindrical open-ended substrate integrated waveguide cavity, the odd TEM mode generated by loading two rectangular via holes inside the cavity, and the higher-order loop modes (L3 and L5) of a circular ring detached from the cavity by a circumferential slot located at the cavity’s side wall. In the implementation of the antenna, slot coupling feeding methodology is applied, which also introduces a resonance for the bandwidth enhancement. A simulated fractional impedance bandwidth of 57.3% with $|{\mathrm{ S}}_{11}| dB from 24.9 GHz to 44.9 GHz is achieved ( $|{\mathrm{ S}}_{11}|= -9.7$ dB at $f=27.7$ GHz is ignored). The antenna has a broadside radiation pattern within the operating frequency band and a maximum simulated broadside gain of 10.6 dBi at ${f}=27$ GHz. Multi-layer technique and metallized via holes processing, which become commercial nowadays, are two critical techniques of the presented antenna. The simple structure is benefit of the fabrication and the integration with other planar front-end circuits. The antenna is fabricated and experimentally verified. A small difference is observed between the measurement and the simulation. A measured fractional bandwidth of 52% from 27 GHz to 46 GHz ( $|{\mathrm{ S}}_{11}|= -9$ dB at ${f}=29$ GHz is ignored) and a measured maximum broadside gain of 9.5 dBi are achieved.

Highlights

  • A composite cavity-based antenna is proposed and presented in this work

  • The higherorder loop modes L3 and L5 respectively resonate at f=25.8 GHz and f=43 GHz, which are close to the resonance frequency of the odd TEM mode or the TE111⁄2 mode

  • It is promising to obtain a wide bandwidth by merging the higher-order loop modes L3, L5 of the circular ring, odd TEM mode of the grounded via holes, and TE111⁄2 mode of the cylindrical open-ended SIW cavity

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Summary

Cavity Model Analysis of Cylindrical Open-Ended Cavity

As investigated in [22], a completely closed cylindrical cavity was applied in the design of wideband antenna because of the versatile mode distribution in the interested band. The mode chart, which shows the mode distribution, is helpful for predicting the bandwidth performance and radiation behavior of an open-ended cavity. The resonant frequency of the dominant TE111⁄2 mode for a cylindrical open-ended cavity with a=3.25 mm, d=1.27 mm, and permittivity of ɛr=2.92 is f=38 GHz. The variation of the resonant frequency verse the changing radius or height is given according equation (3). While the cylindrical open-ended cavity is working in the TE111⁄2 mode, changing the cross-sectional dimension is not as efficient as changing the height to adjust the resonant frequency. Based on the mode chart of the cylindrical open-ended cavity, the achievable bandwidth is quite limited because the available modes are just a few. Multi-layer technique is used to detach a resonant circular ring from the cylindrical open-ended SIW cavity for the bandwidth enhancement

Two Via Holes and Odd TEM Mode
Optimal Dimension of Cavity to Realize High Gain and Wide Bandwidth
Verification by Eigen Mode Analysis
CYLINDRICAL OPEN-ENDED SIW CAVITY ANTENNA WITH RECTANGULAR VIA HOLES
Break-down analysis and parametric study
Important parameters to improve impedance matching
CONCLUSION
Full Text
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