具有双频段过响应的元材料形光束天线
Xianfeng Tang1, Junli Lu2, Xiangqiang Li2
1School of Physical Science and Technology, Southwest Jiaotong University (SWJTU), Chengdu, 611756, China. txf_2012@163.com.
Scientific reports
|May 4, 2025
概括
一个新的超材料 (MTM) 天线提供双频段过和形光束. 这种紧的设计整合了过,减少了对外部组件的需求,并实现了高效的双频段操作.
科学领域:
- 电磁学和天线设计
- 超材料和新材料的使用
- 微波工程 微波工程
背景情况:
- 超材料 (MTM) 具有独特的电磁性质.
- 天线设计通常需要单独的过元件,增加复杂性和尺寸.
- 通过过和特定的辐射模式实现双频段运行提出了设计挑战.
研究的目的:
- 提出一种新型的形光束天线,采用双频段过功能.
- 为了利用超材料的特性进行集成过和紧的天线设计.
- 为了证明基于超材料的天线的可行性,用于双频,形辐射应用.
主要方法:
- 使用超材料 (MTM) 结构设计和模拟一个形光束天线.
- 同轴料和探针合器的集成,用于双频段过.
- 实现一个圆柱形探针用于形光束的产生.
- 拟议的MTM天线的制造和实验测量.
主要成果:
- 拟议的天线展示了以3GHz和4.3GHz为中心的双操作频段.
- 超材料 (MTM) 结构提供了固有的双带过特性.
- 该天线具有紧的横向尺寸,大约为 λ1/7 和 λ2/5.5.
- 测量结果与模拟结果一致,带外增强抑制为~30dB.
结论:
- 开发的超材料 (MTM) 天线成功地集成了双频段过和形束辐射.
- 紧和波器集成的设计消除了对外部波器组件的需求.
- 拟议的MTM天线对于需要双带过和形辐射模式的应用是一个可行的解决方案.
相关概念视频
Parallel Resonance
173
The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
173
Active Filters
677
Active filters are electronic circuits that use operational amplifiers (op-amps), resistors, and capacitors to filter out unwanted frequency components from a signal. A first-order low-pass active filter is designed to pass signals with a frequency lower than a certain cutoff frequency and attenuate frequencies higher than that cutoff frequency. The transfer function for a first-order low-pass active filter is:
677
Passive Filters
420
Passive filters are utilized to shape the frequency spectrum of signals across a diverse array of applications. These filters, using only passive elements like resistors (R), inductors (L), and capacitors (C), are capable of selectively allowing or blocking certain frequency ranges without the need for external power sources.
Low-Pass Filters
Low-pass filters are designed to transmit signals with frequencies lower than the cutoff frequency, ωc, and attenuate those above it. The cutoff...
Low-Pass Filters
Low-pass filters are designed to transmit signals with frequencies lower than the cutoff frequency, ωc, and attenuate those above it. The cutoff...
420
Characteristics of Series Resonant Circuit
192
Series resonance occurs in a circuit containing inductive (L), capacitive (C), and resistive (R) elements connected sequentially. At the resonance frequency, the inductive and capacitive reactances are equal in magnitude but opposite in sign, effectively canceling each other. This causes the circuit's impedance is minimal, primarily determined by the resistance R. The resonant frequency of an RLC circuit is defined as:
192
Mesh Analysis for AC Circuits
309
In the domain of radio communication, the significance of impedance matching must be considered. It is crucial to ensure the efficient transmission of signals between radio transmitters and receivers. Achieving this balance involves using impedance-matching circuits, with one fundamental configuration comprising a resistor, capacitor, and inductor.
The process of harmonizing these impedances begins with a clear understanding of the input and output signals. Once these signals are known, the...
The process of harmonizing these impedances begins with a clear understanding of the input and output signals. Once these signals are known, the...
309
Bandpass Sampling
141
In signal processing, bandpass sampling is an effective technique for sampling signals that have most of their energy concentrated within a narrow frequency band. This type of signal is known as a bandpass signal. The key principle of bandpass sampling involves sampling the signal at a rate that is greater than twice the signal's bandwidth to prevent aliasing.
A bandpass signal has a spectrum with a lower frequency limit, denoted as ω1, and an upper frequency limit, denoted as ω2....
A bandpass signal has a spectrum with a lower frequency limit, denoted as ω1, and an upper frequency limit, denoted as ω2....
141


