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首页> 中文期刊> 《物理学报》 >基于量子相干效应的无芯射频识别标签的r空间散射场测量

基于量子相干效应的无芯射频识别标签的r空间散射场测量

         
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摘要

Chipless radio frequency identification tags have been widely used in many areas, such as vehicle recognition and identification of goods. Near-field measurement of a chipless radio frequency identification tag is important for offering the precise spatial information of the backscattered field of tag. In this paper, we demonstrate the angle discrimination of a line-shape chipless radio-frequency identification tag via the near-field measurements of scattered electric fields in two orthogonal directions. Two laser beams with different frequencies counter propagate and pass through a room-temperature caesium vapor. A Rydberg ladder-type system is formed in the experiment, which includes three levels, namely 6S1/2, 6P3/2, 51D5/2. The electromagnetically induced transparency of transmission of probe light, which is locked to the transition of 6S1/2 ?6P3/2, is observed when the frequency of coupling light varies nearby the transition of 6P3/2 ? 51D5/2. When the 5.366 GHz microwave electric field that is resonant with the transition between two adjacent Rydberg states 51D5/2 ?52P3/2 is applied to the caesium vapor cell by using a standard-gain horn antenna, the transmission signal of probe laser splits into two peaks, which is known as Autler-Townes splitting. The splitting between the transmission peaks is proportional to the microwave electric field strength at the position of laser beam. The spatial distribution of backscattered microwave electric field of the chipless radio-frequency identification tag is obtained through varying the position of the laser beam. The spatial resolution of near-field measurement approximately equalsλMW/12, whereλMW is the wavelength of the measured microwave electric field. The distributions of the electric field strength in two orthogonal directions show the clarity difference while the angle of radio-frequency identification tag is changed. The scattered electric field strength of the identification tag is strongest when the angle of line-shape tag is the same as that of the polarization of the horn antenna. Moreover, the scattered field strength of identification tag in the incident field direction of the horn antenna increases as the measured position and the identification tag get closer to each other. The scattered electric field distributions in the vertical direction are almost constant at the different angles between the incident electric filed and identification tag. The fluctuation of spatial distribution of the scattered electric field strength is attributed to the Fabry-Pérot effect of microwave electric field in the vapor cell. And the geometry of vapor cell results in the minor asymmetric distribution of scattered field. The simulation results from the electromagnetic simulation software are accordant with the experimental results. The novel approach to near-field measurement of identification tag will contribute to studying and designing the chipless radio-frequency identification tag and complex circuits.%基于原子蒸汽池中铯里德伯原子的电磁感应透明光谱在微波场作用下的Aulter-Towns效应,测量了无芯射频识别标签线形散射单元的近场散射微波电场二维空间分布,空间分辨率可达到亚微波波长.实现了射频电场极化方向与线形散射体标签夹角的有效分辨.电磁仿真软件的仿真结果与实验测量符合得很好.本研究提供了一种测量微波电场近场测量的新方法,对无芯射频识别标签的散射单元设计和标定以及电子电路的电磁辐射测量具有重要的意义.

著录项

  • 来源
    《物理学报》 |2017年第24期|32-38|共7页
  • 作者

    闫丽云; 刘家晟; 张好; 张临杰; 肖连团; 贾锁堂;

  • 作者单位

    山西大学物理电子工程学院,太原 030006;

    山西大学激光光谱研究所,量子光学与光量子器件国家重点实验室,太原 030006;

    极端光学协同创新中心,太原 030006;

    山西大学激光光谱研究所,量子光学与光量子器件国家重点实验室,太原 030006;

    极端光学协同创新中心,太原 030006;

    山西大学激光光谱研究所,量子光学与光量子器件国家重点实验室,太原 030006;

    极端光学协同创新中心,太原 030006;

    山西大学激光光谱研究所,量子光学与光量子器件国家重点实验室,太原 030006;

    极端光学协同创新中心,太原 030006;

    山西大学激光光谱研究所,量子光学与光量子器件国家重点实验室,太原 030006;

    极端光学协同创新中心,太原 030006;

  • 原文格式 PDF
  • 正文语种 chi
  • 中图分类
  • 关键词

    电磁感应透明效应; 里德伯原子; 无芯射频识别标签; 反向散射电场;

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