Amplitude-Modulated Dielectric Waveguide for High-Gain Beam Shaping
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Solution Overview
Problem
Existing leaky-wave antennas face challenges in efficiently generating desired radiation patterns due to limitations in amplitude and phase modulation, particularly in converting phase information into amplitude variations for far-field high-gain beam generation and near-field focusing applications.
Innovation Solution
The development of amplitude-modulated leaky-wave antennas using holographic theory, where the intensity of the interference pattern between an object wave and a reference wave is recorded in the wave-guiding structure, allowing for sinusoidal amplitude modulation of the dielectric waveguide's width to generate both amplitude and phase information, enabling high-gain pencil beam and near-field focusing capabilities.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Ease of manufacture
If conventional leaky-wave antennas use uniform wave-guiding structures, then the structure is simple to manufacture, but the radiation pattern control and beam shaping capability are limited
Solution Approach 1:
The patent applies local quality by varying the width of the dielectric waveguide at different positions along its length. Specifically, the waveguide width is modulated according to a sinusoidal function, creating different local geometries that correspond to different radiation characteristics. This allows different sections of the antenna to contribute differently to the overall radiation pattern, enabling beam shaping and focusing capabilities while maintaining a relatively simple integrated structure.
2Adaptability or versatility
If the dielectric waveguide width is varied to achieve amplitude modulation, then the beam shaping and focusing capability is improved, but the manufacturing precision requirements increase
Solution Approach 1:
The patent employs parameter changes by systematically varying the waveguide width parameter along its length according to a mathematical function (sinusoidal modulation). The width w(z) is defined as w0[1 + m*cos(2πζz/L)], where m is the modulation index and ζ is the spatial frequency. This functional approach to parameter variation allows for predictable and controllable beam shaping while providing clear design guidelines for manufacturing tolerances.
3Adaptability or versatility
If holographic theory is used to record interference patterns in the waveguide, then the phase information conversion to amplitude variations is achieved, but the device complexity increases
Solution Approach 1:
The patent applies copying by recording the intensity pattern of an optical hologram into the geometric structure of the dielectric waveguide. The waveguide width modulation profile is essentially a copy of the holographic interference pattern, which encodes both amplitude and phase information of the desired radiation pattern. This allows the antenna to reproduce the complex wavefront characteristics without requiring complex feeding networks or additional active components.
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
This approach allows for the effective generation of high-gain pencil beams and focused near-field electromagnetic power, enhancing the antenna's performance in millimeter-wave bands and enabling applications in 5G communications, radar systems, and non-contact sensing.
Implementation Method 1
a dielectric waveguide extending along the axis and arranged in the substrate
Implementation Method 2
The distance defined between the opposite sides varies along the axis for at least part of a length of the dielectric waveguide
Data Source
AI summary
A leaky-wave antenna includes a substrate extending along an axis, and a dielectric waveguide extending along the axis and arranged in the substrate. The dielectric waveguide includes at least a top side, a bottom side, and opposite sides arranged between the top and bottom sides. A distance defined between the opposite sides varies along the axis for at least part of a length of the dielectric waveguide.


