“…These cases include the linearly-polarized modes, such as the longitudinally-polarized Anisimkin Jr. modes (AMs), with a dominant longitudinal displacement component U 1 with a constant amplitude along the whole depth of the plate, the shear components, U 2 and U 3 , being at least 10-times less than U 1 at any plate depth. AMs were first discovered in quartz plates [ 1 ] and then in LiNbO 3 , Te [ 2 ], LiTaO 3 , Ba 2 NaNb 5 O 15 , KH 2 PO 4 , Li 2 B 4 O 7 , TeO 2 , PbMoO 4 , KH 2 PO 4 and ZnO [ 3 , 4 ] and, recently, in GaPO 4 [ 5 ]. The AMs, while having a phase velocity close to that of the longitudinal bulk acoustic wave (LBAW) traveling in the same direction, can be suitable for the development of high-frequency electroacoustic devices if implemented on fast materials, such as BN and AlN.…”