“…Magnetospheric flow shears are expected, for instance, on closed field lines near the plasmasphere and near the edges of plasmaspheric plumes, especially when hot plasmasheet plasma is injected in the inner magnetosphere during a substorm (McIlwain, 1974;Newell and Meng, 1987;Baker and McPherron, 1990), and in the low latitude boundary layer where the antisunward flow of magnetosheath plasma interfaces with the magnetospheric plasma (Lundin and Evans, 1985;Feldstein et al, 2001;Echim et al, 2008), but also in the plasmasheet (Galperin and Feldshtein, 1989;Baumjohann et al, 1990;Angelopoulos et al, 1992;Chen et al, 2000;Figueiredo et al, 2005;Hamrin et al, 2006;Marghitu et al, 2006;Liléo et al, 2008;Johansson et al, 2009). A second type of electric fields are charge separation electric fields, possibly strengthened by the presence of shear flows, especially at interfaces between cold (plasmasphere/plasmatrough or lobe) and hot (plasmasheet) plasmas, as invoked for discrete arc and subauroral ion drift generators (Ejiri et al, 1980;Feldstein and Galperin, 1985;Yeh et al, 1991;Roth et al, 1993;Lemaire et al, 1998;De Keyser et al, 1998;De Keyser, 1999Johansson et al, 2006;Echim et al, 2007); such fields are capable of creating fine scale structure. Charge separation fields are typically produced at an interface between plasmas with different temperatures or composition: Because their gyroradii are different, exact charge neutrality is impossible to achieve in the interface (Roth et al, 1996).…”