double-barrier resonant-tunneling system. Below a certain threshold voltage V 1, the
charging effect of a single electron in the ultrasmall confinement makes the tunneling current
I 0= 0 at very low temperature. As the voltage V rises above V 1 but below V 2 at which the
charging energy is overcome, the first step of current I 1 shows up. When V becomes even
greater than V 2, both the charging energy and the Coulomb repulsion between two …