Katabatic winds are a common feature of the Antarctic coastline (King & Turner, 1997;Parish & Bromwich, 1987). Longwave radiation from the Antarctic ice sheet cools the snow surface and removes heat from the near-surface air, creating ubiquitous, strong, low-level temperature inversions (Connolley, 1996). The shallow cold air flows downhill and is funneled into coastal valleys, where the sloping terrain allows the air parcels to gain momentum from gravity. In many situations, particularly on the East Antarctic Coast, the katabatic winds peter out quickly beyond the generating slopes due to surface friction, gravity wave dispersion (Renfrew, 2004;Vignon et al., 2020), opposing thermal winds from the build-up of cold air at the slope bottom (Vihma et al., 2011), opposing synoptic forcing (Seefeldt et al., 2007), or entrainment from above the jet (Manins & Sawford, 1979). In some situations, the synoptic pressure gradient forcing is favorable (downstream) or weak (Bromwich et al., 1990;Seefeldt & Cassano, 2012;Seefeldt et al., 2007) or the winds are decoupled from the surface (Andreas et al., 2000) and katabatic winds are able to propagate hundreds of kilometers across flat ice shelves and ocean surfaces.The Antarctic katabatic winds have been the source of considerable attention from the time of the first explorers due to their major impacts on navigation, visibility and human survival. The katabatic winds often form strong jets that are characterized by low-level, high-wind-speed cores that are surrounded by regions of strong vertical and horizontal wind shears. Katabatic jumps, or rapid increases in wind speed associated with the onset of a katabatic wind event (Ball, 1956), are common phenomena in many Antarctic coastal regions (e.g., Vignon et al., 2020). Katabatic winds can extend over the ocean and trigger mesoscale cyclones and other atmospheric features that affect regions far from the initial katabatic wind source (Bromwich,