“…For instance, negative differential conductance can appear [Esaki & Tsu, 1970] (see Fig.1(b)). Thus, semiconductor superlattices can be used as generators of current oscillations, whose frequency depends on the parameters of the superlattice structure and the applied voltage, and thus, can be varied in a wide range from some hundred kHz [Cadiou et al, 1994;Hofbeck et al, 1996;Kastrup et al, 1995;Wang et al, 2000] to hundreds of GHz [Schomburg et al, 1999], which makes this system very promising for practical applications. On the other hand, the inherent nonlinearity gives rise to complex spatio-temporal dynamics of the charge density and the field distribution within the device, including the formation of travelling charge accumulation and depletion fronts and field domains associated with current oscillations.…”