Design and implementation of a 2.8‐dB insertion loss v‐band bandpass filter in 0.13‐μm cmos technology

Abstract

In this article, we demonstrate a low‐insertion‐loss V‐band bandpass filter with two finite transmission zeros by 0.13‐μm CMOS technology. The proposed filter architecture has the following feature: The low‐frequency transmission‐zero (ωz1) can be tuned individually by the series‐feedback capacitor Cs and the series capacitor C3. After ωz1 is determined by Cs and C3, the high‐frequency transmission zero (ωz2) can be tuned individually by the parallel‐feedback capacitor Cp. Besides, low‐insertion‐loss is achieved by adopting thick microstrip‐line with optimized ground‐plane pattern as the needed inductors to minimize the metal and substrate loss. This filter achieves insertion‐loss (1/S21) lower than 3 dB over the frequency range of 45–52 GHz, input return loss (S11) better than −10 dB over the frequency range of 41.2–57.8 GHz, and output return loss (S22) better than −10 dB over the frequency range of 39.5–55.9 GHz. The minimum insertion‐loss is 2.8 dB at 48 GHz, to the authors' knowledge, this is one of the best results ever reported for a V‐band CMOS bandpass filter in the literature. The chip area is only 0.295 × 0.21 mm2, i.e., 0.062 mm2, excluding the test pads and dummy metals for design rule requirement. © 2012 Wiley Periodicals, Inc. Microwave Opt Technol Lett 54:2001–2006, 2012; View this article online at wileyonlinelibrary.com. DOI 10.1002/mop.26984

Estimation of signal attenuation in the 60 GHZ band with an analog BiCMOS passive filter

“…LC filter configurations are the most generally used filters; however, at higher frequencies the bandwidth of the filter depends on the Q -factor of the LC, which could be a limiting factor depending on the technology process. Low insertion loss planar filter structures have been proposed in [4, 5]; however, including two additional inductors to move the high-frequency transmission zero to a finite frequency, increases the already large chip area. In this paper, transmission lines were used as the (inductive) passive components (as opposed to larger spiral inductors) as the high-frequency operation permits practical geometries of these components.…”