I. Introduction
Traditional commercialized 60-GHz radios have been designed as an assembly of several microwave monolithic integrated circuits (MMICs) in gallium arsenide (GaAs) semiconductor technology. They have been used for Gigabit Ethernet (1.25 Gb/s) bridges between local area networks [1], [2]. Recently, integrated transmitter (Tx) and receiver (Rx) MMICs in 0.15- GaAs pHEMT and mHEMT processes have been realized to support data rates of several Gb/s for 60-GHz short-range applications [3], [4]. However, the 60-GHz radios in GaAs MMICs are expensive and bulky. In order for 60-GHz radios to have mass deployment and meet consumer marketplace requirements, the cost and size of any solution must be low and compact. That implies silicon, not GaAs as the better technology choice. In fact, designs towards low-cost highly integrated 60-GHz radios have been realized in silicon technologies. For example, Floyd, et al. have demonstrated a 60-GHz Tx and Rx chipset in a 0.13- silicon-germanium (SiGe) technology [5] and Tanomura, et al. in a 90-nm complementary metal oxide semiconductor (CMOS) technology [6]. An examination of the above works and many other reported 60-GHz highly integrated radios in SiGe and CMOS reveals that two types of antenna-circuit interfaces as shown in Fig. 1 can be identified in the current two-chip solutions. The first type features the 50- single-end and the second type the 100- differential antenna-circuit interfaces. For the first type, the 60-GHz on-chip input/output pads are designed as the ground-signal-ground (GSG) pads; while for the second type as the ground-signal-ground-signal-ground (GSGSG) pads. The GSG pads are bonded to an off-chip but in-package single-end antenna; while the GSGSG pads a differential antenna with either flip-chip or wire-bonding techniques [7]–[10].
Illustration of the (a-b) single-end and (c-d) differential antenna-circuit interface in current highly integrated 60-GHz radios.