Electron transport in electrically biased inverse parabolic double-barrier structure

Bati M^{1, 2, 3, †,}, Sakiroglu S¹, Sokmen I¹

Transmission coefficient as a function of electron energy calculated for two different (a) height asymmetries (V_L = 100 meV and V_L = 125 meV) and (b) thickness asymmetries (W_L = 1 nm and W_L = 2.5 nm). We set L_W = W_R = 5 nm and V_R = 150 meV.