I. Introduction
The rapid development of 5G/6G communication technology has led to extensive research on millimeter-wave (mm-wave) phased arrays. In the mm-wave frequency range below 60 GHz, the method of constructing phased arrays using beamforming chips has been widely used [1], [2], [3], [4], [5], [6], [7], [8], [9], [10], [11], [12], [13], [14], [15]. The phased array based on this architecture requires a power-dividing network to provide power combination or distribution for all chip units. The power-dividing network is most commonly composed of a cascade of Wilkinson power dividers [1], [2], [4], [5], [6], [7], [10], [12], [13]. However, the current Wilkinson network suffers from two disadvantages: first, the transmission lines used in the Wilkinson power dividers are often in the form of strip lines [2], [4], [6], microstrip lines [6], or coplanar waveguides (CPWs) [5], [10], [12], [13], which result in high transmission loss and generally require an RF driver [8] to compensate for the additional line loss. Second, some designs of the Wilkinson network use the buried resistance process [2], which requires an expensive substrate. Surface mount device (SMD) resistors are usually connected by via holes to avoid the buried resistance process.