I. Introduction
Radio frequency (RF) acoustic devices are widely used as sub-6 GHz front-end filters [1], [2], [3], [4]. Acoustic resonators, i.e., key building blocks for filters, piezoelectrically convert the electromagnetic (EM) energy to mechanical vibrations and efficiently store energy at resonances. Such transduction offers two key advantages over EM counterparts, namely, miniature footprints and better frequency selectivity [2]. Among different piezoelectric RF acoustic platforms, current commercial FBARs have been dominated by sputtered aluminum nitride (AlN) and scandium aluminum nitride (ScAlN) since they possess good acoustic properties high-quality factor (), and electromechanical coupling () and their well-established microfabrication process that can be integrated into semiconductor industries effortlessly [2], [5].