概括
这项研究介绍了一种用于多频段,多极化操作的新型超表面天线设计. 创新的天线实现了毫米波通信和雷达系统的高收益.
科学领域:
- 电磁学和应用物理学
- 天线工程天线工程
- 超材料科学科学 超材料科学
背景情况:
- 超表面天线为先进的无线应用提供了潜力.
- 同时实现高增益,多频段运行和极化多样性仍然是一个挑战.
研究的目的:
- 为了介绍一种新的高收益超表面天线设计.
- 为了实现多带操作和多个线性偏振.
- 为了简化超表面天线的设计过程.
主要方法:
- 一个Fabry-Pérot (F-P) 腔与双层超表面传输阵列的集成.
- 基于FP腔的等效焦距的简化设计公式的开发.
- 利用一个独特的单元单元与六个矩形元素的极化多样性和减少金属面积.
- 整合一个宽带堆叠补丁天线与表面波抑制元材料地面平面的宽带堆叠补丁天线.
主要成果:
- 一个制造的原型 (80毫米×80毫米) 实现了20.2dBi和22.7dBi的峰值增益.
- 该天线在23.5-29.2 GHz的广泛带宽上演示了多频段操作.
- 实现了峰值增强频率和偏振控制的动态重新配置.
结论:
- 拟议的超表面天线设计成功地整合了高收益,多频段操作和极化多样性.
- 简化的设计方法和独特的单元细胞有助于优化和紧的天线结构.
- 该天线显示出毫米波通信和雷达系统的巨大潜力.
相关概念视频
NMR Spectrometers: Overview
NMR spectrometers consist of a strong magnet, a radiofrequency transmitter, and a detector attached to a computer console for recording spectra of samples containing NMR-active nuclei. In first-generation NMR instruments called continuous-wave spectrometers, the resonance frequencies of the nuclei are determined by frequency-sweep or field-sweep methods. The magnetic field strength is fixed and the rf signal is swept in the former, while the radiofrequency signal is fixed and the magnetic field...
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences
A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
Standing Waves in a Cavity
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:


