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Volume-Controlled, Two-Carrier Currents in Solids: The Injected Plasma Case
215
Citations
10
References
1961
Year
EngineeringSemiconductor PhysicsPlasma PhysicsInjected Plasma CaseDouble InjectionCharge TransportSemiconductor DeviceSemiconductorsNanoelectronicsCharge Carrier TransportSemiconductor TechnologyElectrical EngineeringInjection LevelPhysicsBias Temperature InstabilityApplied Plasma PhysicMicroelectronicsApplied PhysicsCondensed Matter PhysicsTheoretical StudiesPlasma ApplicationElectrical InsulationBimolecular Recombination Kinetics
Double injection into semiconductors and insulators is examined under conditions where the injected carriers form a free plasma, the current is volume‑controlled by distributed space charge, and the transport is field‑driven with negligible diffusion. The study finds that in extrinsic semiconductors the current follows a J∝V² law over an extended voltage range and is depressed at fixed voltage by increased thermal minority carriers (J∝|n_T−p_T|), a behavior driven by recombination kinetics, while in insulators the current scales as J∝V³, and a rigorous constant‑lifetime solution—also applicable to variable‑lifetime cases such as bimolecular recombination—provides a good approximation for both materials.
Double injection into semiconductors and insulators is studied under conditions where the injected electrons and holes are free (injected plasma), the current is volume-controlled, i.e., determined by distributed space charge, and the current is field-driven (diffusion negligible). The major results are, assuming a one-dimensional geometry and carrier lifetime independent of injection level, for extrinsic semiconductors, (i) an extended voltage region over which $J\ensuremath{\propto}{V}^{2}$ ($J$ current density and $V$ voltage), and (ii) depression of the current, at fixed voltage, in the square-law region through increase in the number of thermal minority carriers, $J\ensuremath{\propto}|{n}_{T}\ensuremath{-}{p}_{T}|$, with ${n}_{T}$, ${p}_{T}$ the thermal-equilibrium densities of electrons and holes, respectively. This unusual behavior is shown to be a direct consequence of recombination kinetic requirements. For insulators, assuming trapping is negligible, $J\ensuremath{\propto}{V}^{3}$. A rigorous solution is obtained for the constant-lifetime problem, valid for both semiconductors and trap-free insulators. This solution furnishes a good approximation also for variable-lifetime cases, e.g., bimolecular recombination kinetics.
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