甚高频和超高频机械耦合氮化铝MEMS滤波器

R. Olsson, C. Washburn, J. Stevens, M. Tuck, C. Nordquist
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引用次数: 27

摘要

本文报道了窄带、后cmos兼容的氮化铝(AlN) MEMS滤波器在甚高频(VHF)和超高频(UHF)频段的发展。利用机械耦合滤波器架构实现了小于0.1%的带宽,其中四分之一波长的光束连接在低速耦合位置,用于连接两个AlN环形谐振器。通过将环上耦合光束的连接移动到共振时不同速度的位置,滤波器带宽成功地从0.09%变化到0.2%。以99.5 MHz为中心,终端阻抗低至200 ω的滤波器的插入损耗为11 dB。利用无源温度补偿技术,这些滤波器的频率温度系数(TCF)已从-21 ppm/C降至2.5 ppm/C。减小的TCF对于窄带宽滤波器至关重要,与未补偿滤波器的100%相比,仅需要13%的滤波器带宽来考虑军用范围(-55至125℃)的温度变化。工作在557 MHz的滤波器是通过环形谐振器和耦合波束的泛音操作实现的,由于谐振器质量因子有限和带宽设计窄,在50 ω时的插入损耗高达32 dB。泛音操作允许实现全差分和平衡型滤波器,其中阻带抑制高达38 dB,尽管插入损耗增加。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
VHF and UHF mechanically coupled aluminum nitride MEMS filters
This paper reports the development of narrow-bandwidth, post-CMOS compatible aluminum nitride (AlN) MEMS filters operating in the very (VHF) and ultra (UHF) high frequency bands. Percent bandwidths less than 0.1% are achieved utilizing a mechanically coupled filter architecture, where a quarter wavelength beam attached in low velocity coupling locations is used to connect two AlN ring resonators. The filter bandwidth has been successfully varied from 0.09% to 0.2% by moving the attachment of the coupling beam on the ring to locations with different velocity at resonance. Insertion losses of 11 dB are obtained for filters centered at 99.5 MHz with low termination impedances of 200 Omega. Utilizing a passive temperature compensation technique, the temperature coefficient of frequency (TCF) for these filters has been reduced from -21 ppm/C to 2.5 ppm/C. The reduced TCF is critical for narrow bandwidth filters, requiring only 13% of the filter bandwidth to account for military range (-55 to 125 C) temperature variations compared to 100% for uncompensated filters. Filters operating at 557 MHz are realized using overtone operation of the ring resonators and coupling beam where higher insertion losses of 32 dB into 50 Omega are seen due to the finite resonator quality factor and narrow bandwidth design. Overtone operation allows for the implementation of fully differential and balun type filters where the stop-band rejection is as high as 38 dB despite the increased insertion loss.
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