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Recombination, Generation, and Non-Equilibrium Carrier Dynamics

Manual: General · Subject: Semiconductor Science

Develop the kinetic picture of carrier recombination, lifetime, quasi-Fermi levels, and transient response.

Non-Equilibrium Carrier Populations

Quasi-Fermi levels

Under illumination or injection, electrons and holes may be described by separate quasi-Fermi levels EFnE_{Fn} and EFpE_{Fp}. Their separation is a direct measure of non-equilibrium and is especially important in photovoltaics, LEDs, and high-injection devices.

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Diagnostic quantity

The splitting EFn−EFpE_{Fn}-E_{Fp} often determines the maximum attainable open-circuit voltage in illuminated devices.

Recombination Mechanisms

Radiative, Auger, and trap-assisted processes

Radiative recombination produces photons and is strong in direct-gap materials. Shockley-Read-Hall recombination proceeds through defect states in the gap and is often dominant in imperfect materials. Auger recombination is a three-carrier process important at high carrier densities, especially in narrow-gap semiconductors and lasers.

Major recombination channels

MechanismTypical dependenceCommon importance
RadiativeR∝np−ni2R \propto np - n_i^2Direct-gap optoelectronics
SRHTrap-assisted, lifetime-limitedDefective or compensated materials
AugerOften scales strongly with carrier densityHigh injection, narrow-gap systems

Which recombination process is explicitly defect-mediated?

What does the splitting of quasi-Fermi levels indicate?

Continuity and Lifetime

Carrier continuity

The continuity equation for electrons is ∂n∂t=1q∇⋅Jn+Gn−Rn\frac{\partial n}{\partial t} = \frac{1}{q}\nabla\cdot\mathbf{J}_n + G_n - R_n, with a corresponding equation for holes. In small-signal analysis, lifetimes and diffusion lengths arise from linearization around steady state.

The carrier lifetime is most directly connected to:

Name one reason SRH recombination can dominate in practical materials.