-A comparative simulation study of planar 94 GHz resonators in a typical BiCMOS BEOL stack-up is presented, with the effect of chip passivation included. It is shown that Q-factors of between 3 and 15 can be obtained, depending on transmission medium and ground plane layer choice. Straight half-wavelength and shorted quarter-wavelength microstrip resonators are shown to outperform CPW, GCPW and hairpin resonators, with highest Qfactors obtained where the lowest available metallization layer is used as ground plane. Q-factors of above 10 may also be achieve in the absence of any ground plane in CPW, which may be implemented in processes (such as GaAs or GaN) where multiple metallization layers are not readily available.
IntroductionMillimeter-wave receivers (30 -110 GHz) have found widespread terrestrial commercial application in passive imaging [1] and automotive RADAR [2] due to the compact size and sharp resolution over short distances. Due to congestion in traditional GSM and LTE frequencies, attention is being turned to the under-utilized mm-wave spectrum for short-and medium-range communications applications [3].Monolithic integration of these future systems [4] presents significant cost and size advantages as opposed to waveguide implementations [5], with Silicon-Germanium Bipolar Complementary Metal-Oxide-Semiconductor (SiGe BiCMOS) providing full mixed-signal mm-wave system-on-chip integration possibilities [6]. To enable complex signal routing for system-onchip applications, the back-end-of-line (BEOL) of RFCMOS and BiCMOS feature multiple metallization layers [6] which may be used to implement complex 2.5D distributed elements.A significant drawback to complete on-chip systems is the high losses associated with passive circuitry surrounding the active transistors on the semiconductor wafer [7]. This is especially problematic in the implementation of on-chip filters, since the mid-band filter insertion loss is inversely proportional to the achievable resonator Q-factor [8]. Typical achieved unloaded quality factors (Q-factors) for on-chip resonators at V-and W-band frequencies have been demonstrated only up to 83 [9] for compound transmission line resonators, 43 for shielded transmission line resonators [10], 25 for single transmission line resonators [11] and below 15 for LC tanks [11].