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Tunable 2D Electromagnetic Band-Gap (EBG) Structures based on Micro-Electro-Mechanical Systems (MEMS) for THz frequencies

机译:基于微机械系统(MEMS)的可调谐2D电磁带 - 间隙(EBG)结构,用于THz频率

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Artificial periodic structures, consisting of an assembly of identical or alike elements in one, two or three dimensions, can be engineered in such a way that they exhibit interesting features when interacting with electromagnetic (EM) waves throughout the spectrum. In optics, photonic band-gap (PBG) crystals exhibit band-gaps where the propagation of EM waves is prohibited. Previous research at lower frequencies resulted in the emergence of frequency-selective surfaces (FSS), consisting of resonant metallo-dielectric periodic arrays with pass/stop band characteristics. Other interesting EM properties, such as in-phase reflection and negative index of refraction, have been demonstrated by means of periodic arrays, such as artificial magnetic conductors (AMC) and negative index materials (NIM). Recently, these and other designs have been categorized under the broad term electromagnetic band gap (EBG) structures [1]. Generally, passive EBG structures exhibit static single-frequency response due to their fixed geometry and materials properties. Static multi-frequency operation devices are achievable by appropriately tailoring single-layer as well as multilayered configurations, where various band gaps or resonant modes are obtained [2-3]. However, in many applications it would be desirable to control dynamically the frequency response. Reconfigurable EBG structures, where the frequency response can be adjusted to the application's specific needs at certain moment and situation, without adding new modules, would greatly benefit communication systems (e.g. aerospace, mobile or wireless applications) in terms of flexibility and efficiency. The tunability mechanisms in periodic arrays, such as EBG structures, can be classified into two major groups, namely (1) geometry-tunable and (2) material-tunable devices. The former reconfigures the shape or arrangement of the elements of the array, whereas the latter exploits the tunable properties of certain materials. The first group includes PiN and varactor diodes, as well as micro-electro-mechanical systems (MEMS) [4-7]. In the second group, we can find plasma elements, as well as ferrite, semiconductor and liquid crystals substrates [8-9]. Every tunability method exhibits unique characteristics, has advantages and drawbacks with respect to the other techniques, and therefore, its usefulness depends on the final application. MEMS structures have shown promising performance in switchable [4-6] and tunable [7] periodic arrays.
机译:人工周期结构,在一个,两个或三个维度上包含相同或类似的元件的组件的,可以以这样的方式使得它们在整个光谱中的电磁(EM)波交互时显示出有趣的特性进行工程改造。在光学,光子带隙(PBG)的晶体表现出的带隙,其中EM波的传播是禁止的。在较低频率处以前的研究导致的频率选择性表面(FSS)的出现,由具有通/带阻特性的谐振金属 - 介电周期性阵列。其它有趣的EM特性,诸如同相反射和折射的负折射率,已经由周期阵列,如人工磁导体(AMC)和负折射率材料(NIM)的手段证实。最近,这些和其他设计已经在广义术语电磁带隙(EBG)结构[1]下分类。通常,被动的EBG结构表现出的静态单频率响应由于它们的固定几何形状和材料性质。静态多频操作装置是通过适当地剪裁单层以及多层构型中,其中获得各种带隙或谐振模式[2-3]可以实现的。然而,在许多应用中,希望以动态地控制频率响应。可重新配置的EBG结构,其中,所述频率响应可被调节以在特定时刻和场合的应用的具体需求,而不添加新的模块,将在灵活性和效率方面大大有利于通信系统(例如航空航天,移动或无线应用)。在周期性的阵列,比如EBG结构可调性机制,可分为两大类,即(1)的几何形状可调,(2)材料可调谐装置。前者重新配置的形状或所述阵列的元件的排列,而后者攻击某些材料的调谐性能。第一组包括销和变容二极管,以及微机电系统(MEMS)[4-7]。在第二组中,我们可以发现等离子体的元件,以及铁素体,半导体及液晶的衬底[8-9]。每个可调谐性方法具有独特的特性,都有优点和缺点,相对于所述的其他技术,并且因此,其实用性取决于最终的应用。 MEMS结构已示于切换[4-6]和可调[7]周期阵列有前途的性能。

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