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Semiconductor Fundamentals · Topic 9 of 13

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Semiconductor FundamentalsLesson 9 of 13

PN junction

Where n-type and p-type meet — the building block that conducts in one direction.

What you’ll learn

  • What forms at a p–n interface
  • The depletion region and built-in potential
  • Forward vs reverse bias

Why it matters

The p–n junction is the heart of diodes, solar cells, LEDs, and every transistor.

Explanation

When p-type and n-type material meet, electrons and holes near the interface recombine, leaving a carrier-free 'depletion region' with a built-in electric field. This field opposes further diffusion and sets up a built-in potential.

Applying forward bias (p positive) shrinks the depletion region and lets current flow; reverse bias widens it and blocks current. That asymmetry is rectification.

Visual explanation

p-typen-typedepletion
A p region and n region meeting, with a depletion zone and its internal field arrow at the junction.

Key terminology

Depletion region
The carrier-free zone at the junction.
Built-in potential
The voltage across the depletion region at equilibrium.
Bias
An externally applied junction voltage.

Example

Under forward bias above ~0.7 V, a silicon p–n junction conducts strongly; under reverse bias it blocks.

Common mistakes

Real-world application

Solar cells generate power by separating light-created carriers across a p–n junction.

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PN junction

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Diode

Semiconductor Fundamentals

A single p–n junction packaged as a one-way current valve.

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