Physical review. B, Condensed matter · 2003 · 14 citations · 13 references
EngineeringMaterials SciencePhysicsElectronic MaterialsSemiconductor DevicesSemiconductor MaterialsDopingQuantum WellsSemiconductor Crystal GrowthSemiconductor Device MaterialsSemiconductor HeterostructuresSemiconductor PhysicsActivation EnergyDoped SemiconductorsLocalized StatesLow-temperature GrowthMolecular Beam EpitaxyP-type ConductivityP-type DopingSemiconductor Doping
Electrical conduction in Be \ensuremath{\delta}-doped GaAs structures grown by molecular-beam epitaxy was studied in the temperature range from 10 to 350 K. A Be \ensuremath{\delta}-doped layer and a 1-nm-thick GaAs spacer layer were grown at 520 \ifmmode^\circ\else\textdegree\fi{}C, followed by growth of a 1-nm-thick GaAs layer with a high concentration of excess As and a 5-nm-thick nearly stoichiometric GaAs layer at a temperature close to 150 \ifmmode^\circ\else\textdegree\fi{}C. At low Be doping concentrations, the conduction is n type and thermally activated, occurring in the 1-nm-thick low-temperature-grown GaAs layer. At higher Be doping concentrations, the conduction is p type and thermally activated, resulting from thermal excitation of localized holes to extended states in the \ensuremath{\delta}-doped well. Activation energies for the p-type conduction range around 100 meV, indicating strong localization of holes in \ensuremath{\delta}-doped wells. By further increasing the Be concentration, the activation energy decreases and eventually leads to the metal-like temperature dependence of the conduction at room temperature, suggesting a possible metal-insulator transition. High-temperature limits of the resistivity of insulating samples were found to be close to the value of the quantum unit of resistance, $\frac{1}{2}{h/e}^{2}.$
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Absence of Diffusion in Certain Random Lattices
P. W. Anderson · Physical Review · 1958 · 12.3K citations
Conduction in glasses containing transition metal ions
N. F. Mott · Journal of Non-Crystalline Solids · 1968 · 2.6K citations