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Distributed sources on coplanar waveguides: application to photomixers for THz local oscillators

机译:共面波导上的分布式源:应用于太赫兹本地振荡器的光混合器

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The lack of compact and frequency-agile local oscillators (LO) constitutes a bottleneck in the performance of submillimeter-wave heterodyne receivers (300 GRz to 3 THz). Traditionally, instruments targeting the lower end of the frequency interval use a chain of frequency multipliers [1, 2]. These multiplier chains perform very well below 1 TRz, but the number of stages required to reach frequencies well into the TRz range renders this solution cumbersome, difficult to design, and eventually inefficient. Since their inception [31, photomixers have been proposed as a competitive alternative to the multiplier chain approach. In these devices, the output power is derived from conductivity modulation in a photoconductive material caused by interference of two impinging lasers having different wavelength. An rf current results due to the application of a dc voltage between electrodes deposited on the surface of the material. Several variations of electrode designs have been proposed and implemented to collect the generated rf current. In some of them the electrodes were localized at the center gaps of dipole antenna elements [31, while other designs make use of distributed coupling to planar transmission lines [4]. In fact, none of these designs has been safisfactory for a variety of reasons. The drawback of gap designs is the concentration of significant optical power on a physically small area. This leads to thermal breakdown of the photomixing materials before any substantial if power could be generated. In the case of the distributed design [41, a lack of electromagnetic modeling tools did not allow the optimization of the various configurations. In particular a coplanar stripline (CPS) design was adopted, which was printed on very thick dielectric substrate. This lead to the generation of a power leaking (radiating) structure and consequently the traveling-wave design suffered large losses along the gain region.
机译:缺少紧凑且频率捷变的本地振荡器(LO)构成了亚毫米波外差接收器(300 GRz至3 THz)的性能瓶颈。传统上,针对频率间隔下限的乐器使用一串倍频器[1、2]。这些乘法器链在低于1 TRz的情况下表现非常好,但是达到频率到TRz范围内所需的级数使该解决方案麻烦,难以设计并且最终效率低下。自从他们成立以来[31,光混合器已经被提议作为倍增链方法的竞争性替代品。在这些设备中,输出功率源自光导材料中的电导率调制,该调制是由具有不同波长的两个入射激光的干涉引起的。射频电流的产生是由于在沉积在材料表面的电极之间施加了直流电压。已经提出并实施了电极设计的几种变型以收集产生的射频电流。在其中一些电极中,电极位于偶极天线元件的中心间隙处[31],而其他设计则利用分布耦合到平面传输线[4]。实际上,由于各种原因,这些设计都没有令人满意。间隙设计的缺点是将很大的光功率集中在物理上很小的区域上。这导致光混合材料的热击穿,然后才可能产生大量的电能。在分布式设计的情况下[41],缺少电磁建模工具无法优化各种配置。特别是采用了共面带状线(CPS)设计,该设计印刷在非常厚的介电基片上。这导致了功率泄漏(辐射)结构的产生,因此行波设计沿增益区域遭受了很大的损耗。

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