“…(1), can be as large as δV ∼ 100-500 mV (see discussion below). In QW systems, instead, the bias range where bistability occurs is mainly controlled by the amount of charge n QW that can be stored in a quantum well, δV ≈ en QW /C, where C is the interlayer capacitance [14]. Typical carrier densities in the "charged" and "uncharged" states of a bistable QW system, assessed by magnetic oscillation measurements [15], are on the order of n QW ∼ 10 11 /cm 2 and n QW ∼ 0, respectively.…”