Atmospheric tides are global-scale waves whose periods are an integer fraction of a solar day (Chapman & Lindzen, 1970). The tides are forced primarily by radiative and latent heating effects in the lower atmosphere (Hagan, 1996), but obtain their largest amplitudes in the mesosphere-lower-thermosphere (MLT) region (80-120 km altitude). There they are expressed as pronounced oscillations in a broad range of atmospheric fields, such as density, pressure, and wind. The migrating tides are those tides which follow the apparent motion of the sun, having a longitudinal zonal wavenumber (S) and latitudinal spherical harmonic (Hough mode) structure. In the current work, the focus lies on the migrating semidiurnal (SW2; for Semidiurnal, Westward S = 2) tide. The SW2 tidal winds maximize in the mid-and high-latitude MLT (Manson et al., 2002;Wu et al., 2011), where they form a major source of day-to-day and inter-seasonal variability of the MLT-ionosphere system (Arras et al., 2009;G. Shepherd et al., 1998;Smith, 2012). The SW2 tide is recognized as an important vertical coupling mechanism (Forbes, 2009;Pedatella & Forbes, 2010), and as a contributing factor to the vertical mixing and energy budget of the upper atmosphere (Becker, 2017;Forbes et al., 1993).The numerical study of the SW2 tide has a long history (e.g., Forbes & Garrett, 1979). Nevertheless, open questions remain about the mechanisms governing the tide's seasonal and short-term variability (