← Back to CoursesSemiconductor Science: Intermediate

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Recombination, Generation, and Carrier Lifetime

Manual: General · Subject: Semiconductor Science

Study how carriers are created and destroyed in semiconductors.

Non-Equilibrium Carrier Dynamics

Recombination mechanisms

Electrons and holes can recombine through radiative recombination, Shockley-Read-Hall trap-assisted recombination, or Auger recombination. The dominant pathway depends on material, defect density, and carrier concentration.

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Why defects matter

Crystal defects and impurities create energy levels in the band gap that can greatly accelerate recombination and shorten carrier lifetime.

Lifetime and diffusion length

Carrier lifetime τ\tau describes how long excess carriers persist. The diffusion length is often approximated by L=DτL = \sqrt{D\tau}, linking transport to recombination.

Common recombination paths

MechanismTypical conditionKey idea
RadiativeDirect band-gap materialsPhoton emission accompanies recombination
SRHDefect-rich materialsTrap states mediate recombination
AugerHigh carrier densityEnergy given to a third carrier

Which recombination mechanism is most associated with trap states in the band gap?

What is carrier lifetime?

Using lifetime in device reasoning

  1. 1

    Identify the dominant recombination mechanism.

  2. 2

    Estimate or look up carrier lifetime τ\tau.

  3. 3

    Compute diffusion length with L=DτL = \sqrt{D\tau}.

  4. 4

    Compare diffusion length to device dimensions to judge performance impact.

Direct vs indirect recombination consequences

Direct band-gap materials

  • Efficient light emission
  • Useful in LEDs and lasers

Indirect or defect-rich materials

  • Weaker light emission
  • Often dominated by nonradiative paths

If carrier lifetime decreases while diffusivity stays the same, what happens to diffusion length?

Write the diffusion length relation.