I. Introduction
To overcome the high path losses of millimeter (mm)-wave frequencies and to use beam space multiple inputs and multiple outputs (MIMOs) in wireless communication systems, the phased-array beamforming technique has been widely studied. High-bit phase and gain controls are required to support massive MIMO and to perform phased-array calibrations. Active phase shifters based on vector-summing synthesizers are more advantageous than passive phase shifters based on switches. This is because the active phase shifters allow small insertion loss with a gain control function and high-bit phase and gain resolutions without increased chip size. Passive phase shifters require a chip area that is commensurate with the number of phase control bits and an additional chip size to implement a variable-gain function. Therefore, active phase shifters with gain controls are being intensively studied. Dual vector synthesizers are applied to control gain and phase independently without output impedance changes [1], but they have a small gain control range of ~8 dB, and the gain is deteriorated by the parasitic capacitances of the complex RF structure. An attenuator-based vector sum-type phase shifter [2] provides a high gain control range, but it has large rms phase and gain errors due to discrete attenuations. To drive vector synthesizers, various I/Q generators have also been studied. The delay line-based I/Q generation provides the widest bandwidth, but it has a too large size to take advantage of a high degree of integration of active phase shifters [3]. A classical two-stage RC poly-phase filter (PPF) with small loading effects and wideband characteristics is used as an I/Q generator of the active phase shifter in mm wave bands [4]–[6], but it has a large insertion loss due to impedance mismatches between the stages and the impedance mismatch with the Gilbert cell.