“…The 2D Poisson's equation is solved on the devices of Figure using a parabolic approximation of the 2D potential, ψ i (x, y), where, i = 1, 2, 3, 4 corresponds to regions I (− a ≤ x ≤ 0), II (0 ≤ x ≤ b ), III ( b ≤ x ≤ c ), and IV ( c ≤ x ≤ d ), respectively, of the device, regions I, and IV being the junction depletion regions …”