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Consider a long rectangular bar of direct bandgap p-type semiconductor. The equilibrium hole density is 10¹⁷ cm⁻³ and the intrinsic carrier concentration is 10¹⁰ cm⁻³. Electron and hole diffusion lengths are 2 μm and 1 μm, respectively.
The left side of the bar (x = 0) is uniformly illuminated with a laser having photon energy greater than the bandgap of the semiconductor. Excess electron-hole pairs are generated ONLY at x = 0 because of the laser. The steady state electron density at x = 0 is 0.15 × 10¹⁴ cm⁻³ due to laser illumination. Under these conditions and ignoring electric field, the closest approximation (among the given options) of the steady state electron density at x = 2 μm, is _________.
- 0.37 × 10¹⁴ cm⁻³
- 0.63 × 10¹³ cm⁻³
- 3.7 × 10¹⁴ cm⁻³
- 10³ cm⁻³
Correct answer: 0.63 × 10¹³ cm⁻³
Solution
The steady state electron density at a distance from the generation point can be approximated using the diffusion equation, which accounts for the initial excess electron density and the diffusion length. Given the diffusion length of electrons is 2 μm and the initial density at x = 0 is 0.15 × 10¹⁴ cm⁻³, the density decreases exponentially with distance, leading to a calculated value of approximately 0.63 × 10¹³ cm⁻³ at x = 2 μm.
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