“…3,4 At a higher velocity range between the longitudinal sound velocities of the film (V F L ) and substrate (V S L ), the longitudinal guided mode ͑LGM͒ exists when V F L ϽV S L , and is characterized by mode displacements primarily along the film plane and a phase velocity close to V F L . 5 Excitations lying within these two distinct transverse or longitudinal velocity bands provide for a complete description of acoustic waves in a soft film on a hard material ͑i.e., V F T ϽV S T ͒, and have been extensively studied. [6][7][8][9][10] In the opposite limit, i.e., for hard films deposited on soft substrates (V S T ϽV F T ), only one surface acoustic wave ͑SAW͒, identified as the Rayleigh wave, exists in a narrow velocity range limited by V S T , provided the film thickness ͑h͒ is below a critical value.…”