Planar slotted ridged waveguide antenna arrays with dielectric layer

Author(s):  
A.O. Pelevin ◽  
G.F. Zargano ◽  
A.M. Lerer

The paper simulates the options available to move operating range of slotted waveguide antennas downward in frequency without changing the waveguide cross-section, and suggests the ways for designing linear waveguide-slotted elements based on rectangular and ridge waveguides with air and partial dielectric filling. The critical frequency of the fundamental mode of a 16x8 mm rectangular waveguide moves by ridging from 9.5 to 6.5 GHz. Partial dielectric filling of the cavity of the ridge waveguide makes it possible to additionally shift the operating range downward in frequency by 6-10% without making changes to antenna design. The antenna characteristics of linear arrays based on a dielectric-filled ridge slotted waveguide have been compared in terms of gain and voltage standing wave ratio to similar designs of arrays on rectangular and air-filled analogues. Based on the obtained structures of linear elements, simulation models of planar arrays have been constructed so that they have the similar area of total surface. Simulated frequency dependence of the realized gain for planar arrays has demonstrated a shift of the operating range downward in frequency. The analysis of the directivity characteristics of planar arrays for various phase shifts between the linear elements has been carried out. The simulation results have shown that the use of a dielectric-filled ridge waveguide gives an advantage in phase scan angle of the main beam of the radiation pattern. With the same phase shift, in planar arrays of dielectric-filled ridge waveguides, the main beam scans for a larger angle while keeping side lobes at low level. Thus, the use of a ridge slotted waveguide with a dielectric layer inside makes it possible to expand the phase scan angle.

Antennas ◽  
2021 ◽  
Author(s):  
A. O. Pelevin ◽  
G. F. Zargano

Slotted single-ridge waveguide antenna with dielectric filling has been simulated. Dielectric material has been used to fill the slots, and to form a thin layer directly under the slotted broad wall. The specific pairs of ridge dimensions have been found that provide the same cut-off frequency for an air-filled ridged waveguide as it is for a broader air-filled rectangular waveguide. It has been shown that waveguide ridging followed by insertion of a thin dielectric layer under the slotted wall shift consecutively the antenna operating band down to lower frequencies. The specific values of thickness and permittivity of the dielectric layer suitable for frequency shifting have been found. The simulated characteristics of a 20-element dielectrically filled slotted single-ridge waveguide antenna have been presented. Resultantly, the efficient method of shifting the operating interval of a slotted-waveguide antenna down to lower frequencies has been proposed. The method does not require a broader waveguide, and therefore is effective with respect to low frequency – mass/dimension trade-off.


Author(s):  
A. O. Pelevin ◽  
A. M. Lerer ◽  
G. F. Zargano

The article describes the computer simulation of phased antenna arrays consisting of slotted waveguide antennas with air and dielectric filling. It is shown that inser-tion of a thin dielectric layer shifts the operating frequency range of phased anten-na arrays by 1 GHz or more down in frequency while maintaining directional char-acteristics.


2011 ◽  
Vol 10 (04n05) ◽  
pp. 771-775 ◽  
Author(s):  
DIKSHA MAKWANI ◽  
R. VIJAYA

Planar and ridge waveguides are written on SU-8 thin film, coated on end polished glass substrate, by optical lithography technique at near-UV wavelengths. A significant amount of light from a diode laser at 635 nm is guided down the ridge waveguide in the experiment designed to study optical characterization. The measurement of guiding parameters such as number of modes, depth of the waveguide and refractive index are done using prism coupling technique. Simulation results on beam propagation in the SU-8 ridge waveguide (length of 2.54 cm, width of 10 μm and depth of 6 μm) show an appreciable far-field intensity profile that qualifies the waveguide design.


Author(s):  
Tai-Ho Yu

Abstract This study investigates the dispersive properties of ridge waves that travel circumferentially around piezoelectric circular ridge waveguides and investigates their resonant modes. Based on the variable separation method and Hamilton's principle, the displacement of ridge waveguides is represented as the product of a cross-sectional coordinate-dependent function and the propagator along the circumference of a circular ridge waveguide. The dispersion curves of the flexural waves and resonant frequencies corresponding to ridge waveguides are solved numerically by applying the bi-dimensional finite element method (Bi-d FEM) and using the 3D ANSYS package. The estimated impedance curves are compared with the predicted dispersion curves of waves from ridge waveguides to validate the proposed numerical approach. The geometric parameters and elastic constants of the piezoelectric circular ridge waveguide are determined through an inverse scheme that is based on the measured resonant frequencies and uses the modified simplex method. The numerical and experimental results show that, using the modified simplex method to inverse calculate the elastic constants and geometric parameters of the piezoelectric circular ridge waveguides, a good degree of accuracy and sensitivity can be achieved.


2014 ◽  
Vol 1720 ◽  
Author(s):  
Thomas A. Wall ◽  
Joshua Parks ◽  
Kaelyn D. Leake ◽  
Holger Schmidt ◽  
Aaron R. Hawkins

ABSTRACTWe review an optofluidic waveguiding lab-on-a-chip used to sense bioparticles. The sensor uses a liquid filled Anti-Resonant Reflecting Optical Waveguide (ARROW) that is interfaced with standard ridge waveguides. The ridge waveguides are coupled to off-chip lasers and detectors via optical fiber. A perpendicular intersection between the ARROW and a ridge waveguide is especially useful for detecting fluorescently tagged particles. Light coupled into the ridge waveguide can fluorescently excite these particles within a very small volume. Fluorescent signal can then be guided within the ARROW and subsequently off chip to a detector.We also discuss how such devices are fabricated. Both the ARROW and ridge waveguides are made using alternating thin films of tantalum oxide and silicon dioxide on silicon substrates. These thin films are deposited by either sputtering or plasma enhanced chemical vapor deposition (PECVD). The waveguides are patterned using a combination of standard photolithographic processes, reactive ion etching, and sacrificial etching. Low-loss optical guiding is very dependent on both the waveguide structure and the materials used. The latest processes for maximizing detection sensitivity are reviewed.We also present results using the optofluidic waveguiding sensor for detecting a variety of different types of particles such as fluorescently labeled nanobeads, viruses, ribosomes, and RNA.


Nanoscale ◽  
2019 ◽  
Vol 11 (15) ◽  
pp. 7140-7148 ◽  
Author(s):  
Fengyuan Gan ◽  
Hongyun Li ◽  
Jianjun Chen

The emission polarization is tailored in both the spectral and spatial domains by designing metasurface-based emitters on plasmonic ridge waveguides.


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