Fast latitudinally narrow plasma flows with velocities greater than 1,000 m/s are a common occurrence within the high latitude nightside ionosphere (Archer et al., 2017). Background plasma convection at high latitudes is typically controlled by the interaction between the solar wind and magnetosphere via dayside/nightside magnetic reconnection (Crooker, 1979; Dungey, 1961) and viscous interactions (Axford & Hines, 1961). During intervals of low to moderate solar wind driving, statistical patterns of ionospheric convection flow indicate that auroral zone flows are typically less than ∼600 m/s (Thomas & Shepherd, 2018) and during stronger magnetic activity can reach values exceeding 1,000 m/s (Provan et al., 2004) in the subauroral dusk to pre-midnight region. Fast westward flows in the subauroral pre-midnight region are usually associated with substorms and depending upon their timing, location, and extent relative to substorm onset, are either identified as polarization jets (Galperin, 2002), subauroral polarization streams (SAPS, Foster & Vo, 2002), or subauroral ion drifts (SAIDs, Anderson et al., 1993; Spiro et al., 1979). However, during quiet geomagnetic conditions Archer et al. (2017) have identified recurring latitudinally narrow fast flow jets in the midnight sector of the auroral winter ionosphere that are distinctly different from SAPS and SAIDS. These >1,000 m/s flows are bounded by upward and downward field-aligned currents (FACs) on the order