“…Defining the polarization of the mode is based upon two well-known experimental data [3,11,12]: (i) an acoustic wave, having nonzero vertical displacement U 3 at the liquid/solid interface and large propagation velocity v n as compared with compressional wave velocity in the liquid v lq , is suffered from attenuation a because the wave energy is continuously radiated into the liquid medium--therefore, the magnitude of the U 3 component at the plate surface may be qualitatively estimated for any mode from the value of the attenuation a n measured for water as a liquid with low viscosity g: the less the a n , the smaller the U 3 for a given mode; (ii) an acoustic wave, having nonzero shear-horizontal displacement U 2 at the liquid/solid interface, is suffered from viscoelastic loss increased proportionally to the liquid viscosity g--therefore, the magnitude of the U 2 component at the plate surface may be qualitatively estimated for any mode from the attenuation a n measured for glycerin as a liquid with high viscosity g: the less the a n , the smaller the U 2 for a given mode. As a result, modes, whose attenuation a n is relatively small for both liquids, contain smallest U 3 and U 2 components, and, thereby, might be identified as quasi-longitudinal.…”