“…The major mechanisms include (Eden & Olbers, 2014; Müller et al., 1986; Polzin & Lvov, 2011): (1) interaction with (sub)‐mesoscale ocean turbulence (Duda et al., 2018; Dunphy et al., 2017; Kafiabad et al., 2019; Savva & Vanneste, 2018), (2) scattering by topographic corrugations (Baines, 1971a; Kelly et al., 2013; Müller & Xu, 1992), and (3) nonlinear wave‐wave interactions such as Parametric Subharmonic Instability (e.g., McComas & Bretherton, 1977; MacKinnon et al., 2012; D. J. Olbers, 1976; D. Olbers et al., 2020; Onuki & Hibiya, 2018). As low mode internal tides (typically the first and, to a weaker extent, the second baroclinic modes) can propagate long distances, they lose coherence (which is associated with departure from an exactly repeating signal) through the above‐mentioned processes (Buijsman et al., 2017; B. Li et al., 2020; Nelson et al., 2019) and, in addition, they have a remote impact in the ocean. This greatly complicates the spatial distribution of the internal tide field and its impact in the global ocean, and in particular the distribution of the associated diapycnal mixing (Melet et al., 2016).…”