An isolated nanometre-sized island has small total capacitance , so discrete charge carries appreciable charging energy. A simple constant interaction model is
Away from charge degeneracy, adding or removing an electron costs more energy than a sufficiently small thermal/bias window supplies. Coulomb blockade suppresses sequential tunnelling between resolved charge states.
A single-electron transistor has source and drain reservoirs connected to an island through two tunnel junctions, plus an insulated capacitive gate. Each junction has resistance and capacitance; the gate shifts electrostatic energies without carrying the transport current. The original device schematic labels all components.
Require , a source–drain window below the relevant transition, and junction resistances well above to suppress strong quantum charge fluctuations. Electromagnetic noise and lifetime broadening must also be small. Gate-induced charge degeneracy permits conduction even at small bias; there is no gate-independent blockade threshold. Resolving orbital levels additionally requires temperature and broadening below their spacing between energy levels.
Figure 1.
Single-electron charging and lateral confinement of a heterostructure electron gas
. Original circuit, heterostructure and gate-defined confinement schematics. The band profiles and layer thicknesses are qualitative, not material-specific measurements. Details.

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