In the Earth's inner magnetosphere, which generally lies within L-shell = 7, the cold plasma population (∼1 eV) is divided into three spatial regions: the plasmasphere, the plasma trough, and the plasmasphere boundary layer (PBL). The plasmasphere is a torus-like, high-density (≥50 cc) region around the Earth, while the surrounding plasma trough is tenuous (∼ 1 cc). Between the two regions is the PBL (or the plasmapause), with large density gradients and often accompanied by significant density structures (Carpenter & Lemaire, 2004). The location of PBL, which is controlled by global convection (Chappell, 1972;Nishida, 1966), is highly dynamic in response to geomagnetic activities: it varies from L = 2-3 due to erosion during active conditions (Carpenter & Anderson, 1992;Moldwin et al., 2002) to L ∼ 7 due to refilling during prolonged quiet conditions (Kwon et al., 2015). One large-scale (∼1 R E ) structure near the PBL is the plasmaspheric plume, which is peeled away from the plasmasphere by enhanced convection fields (Chen & Wolf, 1972;Goldstein et al., 2004). Other medium-density to large-density structures (>0.1 R E ) include the notches, channels, shoulders, fingers, and crenulations observed in EUV (extreme ultraviolet) images (Darrouzet et al., 2009;Spasojević et al., 2003).Small-scale density irregularities have cross-field scales ranging from ∼10 m to ∼1,000 km and occur in all parts of the inner magnetosphere (Sonwalkar, 2006). They have been extensively observed in the PBL (Décréau et al., 2005) and plume regions (Borovsky & Denton, 2008;Goldstein et al., 2004). Small-scale density irregularities are generally thought to be field-aligned structures and thus are referred to as field-aligned irregularities