宽带循环偏振磁电双极天线用于毫米波通信
Ting Wu1,2, Chen Zhang1
1Xi'an Key Laboratory of Wireless Optical Communication and Network Research, School of Automation and Information Engineering, Xi'an University of Technology, Xi'an, Shaanxi Province, China.
iScience
|October 31, 2025
概括
这项研究引入了一种新的宽带循环偏振天线,用于毫米波通信. 该设计实现了宽带宽和高收益,适用于先进的无线系统.
科学领域:
- 电磁学和波浪传播
- 天线理论和设计.
- 微波工程 微波工程
背景情况:
- 毫米波 (mmW) 通信系统需要高性能天线.
- 现有的天线通常面临带宽和极化纯度的限制.
- 磁电 (ME) 双极天线为小型化和宽带操作提供了潜力.
研究的目的:
- 提出和演示一个宽带循环极化 (CP) 磁电 (ME) 双极天线.
- 为了提高ME双极天线的带宽和轴比 (AR) 性能.
- 通过模拟和制造用于mmW应用的4x4阵列来验证设计.
主要方法:
- 修改传统的线性极化ME双极,使用中心对称的L形条纹用于CP辐射.
- 在合槽上集成微条线输入与中心对称的匹配分支.
- 包括一个寄生顶层来提高带宽.
- 使用顺序旋转技术 (SRT) 的4x4阵列的制造和测量.
主要成果:
- 单元实现了26.9%的阻抗带宽和20.8%的3dBAR带宽,峰值增益为8dBic.
- 4x4阵列显示了30.7%的阻抗带宽和26.5%的3dBAR带宽,峰值增益为15dBic.
- 对阵列的模拟和测量结果之间观察到很好的一致性.
结论:
- 拟议的天线设计为mmW系统提供了卓越的CP性能和宽带宽.
- 低调和高集成能力使其适合于实际的mmW通信设备.
- 这项工作为下一代高频无线通信天线提供了可行的解决方案.
相关概念视频
Diamagnetism
2.9K
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
2.9K
Standing Waves in a Cavity
1.4K
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:
1.4K
Magnetic Field Due To A Thin Straight Wire
6.0K
Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
6.0K
Potential Due to a Magnetized Object
761
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
The vector...
761
Induced Electric Dipoles
4.7K
A permanent electric dipole orients itself along an external electric field. This rotation can be quantified by defining the potential energy because the external torque does work in rotating it. Then, the potential energy is minimum at the parallel configuration and maximum at the antiparallel configuration. While the former is a stable equilibrium, the latter is an unstable equilibrium.
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...
4.7K
Magnetic Moment of an Electron
2.7K
Electrons revolving around a nucleus are analogous to a circular current carrying loop. This current produces a magnetic dipole moment proportional to the electron's orbital angular momentum. Since the orbital angular momentum is quantized in terms of the reduced Planck's constant, the dipole moment is quantized in the Bohr Magneton. The value of the Bohr magneton is 9.27 x 10-24 Am2. Electrons also have an intrinsic spin angular momentum, and the associated spin magnetic moment is...
2.7K


