I. Introduction
Microacoustic piezoelectric resonators have been pivotal components for the implementation of modern Radio Frequency (RF) communication paradigms [1]. However, research continues to explore the capabilities of micro- and nanoelectromechanical systems (M/NEMS) for cutting-edge applications, particularly within the 5G FR-2 (mmWave) and anticipated FR-3 (X to Ku) bands [2]. In fact, as frequency increases, acoustic losses become more pronounced, hindering the implementation of microacoustic filters beyond 5 GHz. This challenge persists across all proposed technologies, either based on nano-scaled fundamental modes or overtones, and piezoelectric materials [3].