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Lesson: Chapter 11 — Electronics

11.2. The p-n junction 1 of 2

The depletion layer

Dope one side of a silicon or germanium crystal with a group III element (p-type) and the other with a group V element (n-type). Where they meet there is a p-n junction, which behaves quite differently from an ordinary conductor.

Figure to be added

Figure 11.5 — (a) free electrons diffusing from n to p and holes from p to n; (b) the depletion layer, negative on the p side and positive on the n side, as a potential barrier.

As soon as the junction forms, free electrons from the n side diffuse across to the p side and holes from the p side diffuse to the n side. Electrons fill holes, leaving a region near the junction with no carriers.

Depletion layer

That carrier-free region is the depletion layer. Its p side has gained electrons and is negative; its n side has gained positive charge. The potential difference across it repels carriers and stops the diffusion: it is a potential barrier.

Junction Potential barrier
Silicon ≈ 0.7 V
Germanium ≈ 0.3 V