“…In general, this term becomes important when the dimensionless modulation frequency is on the order of, or larger than, the dimensionless attenuation coefficient a ¼ OðeÞ. In the context of plane waves, it was shown (Dontsov and Guzina, 2011a) that the modulationdriven contribution to the ARF can be used to explain the phenomenon of difference-frequency generation (Thuras et al, 1935) of the mean motion in lossless fluids where a ¼ 0. In the literature, the phenomena of difference-frequency generation and ARF were long thought to be unrelated owing to the common notion that the ARF vanishes in homogeneous lossless media (Ostorvsky et al, 2007), as indicated by the formula for g E z,dir in (94).…”