In the high-latitude ionosphere, the primary source regions for plasma structuring tend to be located in the dayside cusp and the nightside auroral oval, where electron precipitation is abundant (Kelley et al., 1982). The large-scale polar convection pattern then causes the structured plasma to travel anti-sunward through the polar cap (Cowley & Lockwood, 1992;Dungey, 1961). In fact, the transport of irregularities from particle precipitation-driven source regions into the polar cap proper is an essential reason for the observed polar cap plasma structures (Cowley, 2000), although alternative sources of structuring inside the polar cap proper exist, such as the gradient drift instability mechanism (e.g., Tsunoda, 1988). Without an irregularity production source, the lifetime of a given plasma structure entering the polar cap is an indicator of the effectiveness with which the plasma structures are diffusing into the surrounding plasma. Indeed, Jin et al. (2017) found that occurrence of plasma irregularities drops significantly when plasma leaves the cusp region.The occurrence of plasma irregularities in the high-latitude regions is in general subject to strong seasonal dependencies (