Depletion Region

The complete guide to the depletion region — the carrier-free space-charge zone at the heart of every PN junction. From how it forms by diffusion and recombination, to the built-in barrier potential, forward vs reverse bias, and junction capacitance.

Complete Learning Path — Depletion Region

From how the depletion region forms, through the barrier potential and bias effects, to its charge/field/potential profile, width and junction capacitance

What is the Depletion Region?

The depletion region — also called the space-charge region or depletion layer — is the thin zone around a PN junction that is emptied of free charge carriers. It is the feature that makes a diode a diode.

When a P-type region (rich in holes) meets an N-type region (rich in electrons), carriers diffuse across the junction and recombine. Left behind are the fixed, charged dopant ions — negative acceptors on the P side, positive donors on the N side — a region with charge but no free carriers.

Formation of the depletion region at a PN junction: electrons and holes diffuse and recombine, leaving fixed acceptor and donor ions
Holes and electrons diffuse across the junction and recombine, leaving fixed acceptor (−) and donor (+) ions — a carrier-free depletion region.
W
Depletion width
Vbi
Barrier potential
0.7 V
Silicon barrier
0.3 V
Germanium barrier
Space charge, but no current

The depletion region contains charged fixed ions but no mobile carriers, so it behaves like an insulating barrier — until an applied voltage changes its width.

Built-in Field & Barrier Potential

Those fixed ions create an internal electric field across the depletion region and a barrier potential that opposes further diffusion — the equilibrium that stabilises the junction.

Built-in electric field pointing N to P and the barrier potential across the depletion region
The fixed ions set up a built-in field (N → P) and a barrier potential Vbi that carriers must overcome to cross.

Vbi = (kT/q) ln(NAND / ni²)  ·  ≈ 0.7 V (Si), 0.3 V (Ge)

Built-in (barrier) potential from the doping levels; k = Boltzmann, T = temperature, q = electron charge

Why a diode “turns on” at 0.7 V

The barrier potential is exactly the forward voltage a silicon diode needs before it conducts strongly — the famous 0.7 V knee.

Forward Bias: the Region Narrows

Connect the battery + to P and − to N and you fight the built-in field. Majority carriers are pushed toward the junction, so the depletion region narrows and the barrier falls.

Forward bias narrows the depletion region so current flows through the diode
Forward bias shrinks the depletion region and lowers the barrier — once V exceeds ~0.7 V, the junction conducts and current flows.
This is how a diode conducts

A forward-biased junction is a low-resistance path — the basis of rectification, LEDs and the “on” state of transistors.

Reverse Bias: the Region Widens

Reverse the battery — + to N and − to P — and you reinforce the built-in field. Carriers are pulled away from the junction, so the depletion region widens and the barrier rises. Almost no current flows.

Reverse bias widens the depletion region and blocks current except a tiny leakage
Reverse bias widens the depletion region and raises the barrier — only a tiny reverse saturation (leakage) current IS flows.
Breakdown

Push reverse voltage too high and the junction breaks down (avalanche or Zener effect), conducting suddenly — deliberately exploited in Zener diodes for voltage regulation.

Charge, Field & Potential Profile

Three graphs across the depletion width tell the whole quantitative story — from fixed charge, to the field it creates, to the potential that results.

Space charge density, triangular electric field and rising potential across the depletion width W
Space-charge density ρ (steps), the resulting triangular electric field (peak at the junction), and the potential rising to Vbi — all across the depletion width W.

Emax at the junction  ·  area under E = Vbi  ·  NAxP = NDxN

Charge neutrality makes the region extend further into the lightly-doped side

Depletion Width & Junction Capacitance

The width W changes with doping and bias — and because the region separates charge like a capacitor, it gives the junction a voltage-controlled capacitance.

Depletion region acting as a capacitor with junction capacitance Cj = epsilon A / W
The carrier-free zone is like a capacitor with plate gap W: Cj = εA/W. Wider reverse bias → larger W → smaller Cj.

W ∝ √(Vbi − V)  ·  Cj = εA / W ∝ 1/√(Vbi − V)

Depletion width and junction (transition) capacitance vs applied voltage

The varactor diode

A reverse-biased junction is a voltage-tunable capacitor — the varactor (varicap) diode, used to tune radios, PLLs and oscillators electronically.

Why the Depletion Region Matters

Almost every semiconductor device works by controlling a depletion region.

Diodes & rectifiers

Its one-way behaviour turns AC into DC in every diode and rectifier.

LEDs & lasers

Recombination across the junction emits light in LEDs and laser diodes.

Solar cells & photodiodes

The built-in field sweeps light-generated carriers apart to make current.

Transistors

BJTs and MOSFETs switch by modulating junction/channel depletion.

Varactors

Voltage-controlled junction capacitance tunes RF circuits.

Zener & breakdown

Controlled reverse breakdown regulates voltage in Zener diodes.

Key Terms at a Glance

The essential depletion-region vocabulary students and engineers search for.

Depletion region

Carrier-free space-charge zone at a junction.

Space charge

Fixed acceptor (−) & donor (+) ions.

Barrier potential

Vbi ≈ 0.7 V (Si), 0.3 V (Ge).

Built-in field

Internal field N → P.

Depletion width W

Thickness; changes with bias.

Forward / reverse bias

Narrows / widens the region.

Junction capacitance

Cj = εA/W.

Leakage current

Tiny reverse IS.

Frequently Asked Questions

Quick, expert answers to the questions people ask most about the depletion region.

What is the depletion region in simple words?

It is a thin layer around a PN junction with no free electrons or holes — only fixed charged ions. Because it has no free carriers, it acts like a barrier that controls whether the diode conducts.

How is the depletion region formed?

Electrons from the N side and holes from the P side diffuse across the junction and recombine, leaving fixed donor and acceptor ions. Their charge builds a field that stops further diffusion, forming a stable carrier-free zone.

What is the barrier potential?

The voltage across the depletion region from the fixed ions: about 0.7 V for silicon and 0.3 V for germanium. A forward voltage must exceed it before the diode conducts.

Does forward bias increase or decrease the depletion region?

Forward bias decreases (narrows) it. Pushing carriers toward the junction lowers the barrier, so above ~0.7 V the diode conducts.

Why does reverse bias widen the depletion region?

Reverse bias pulls majority carriers away from the junction, exposing more fixed ions, so the region grows wider and the barrier gets higher — blocking current except a tiny leakage.

What is the depletion width?

The thickness W of the region. It depends on doping and voltage, extends further into the lightly-doped side, and roughly follows W ∝ √(Vbi − V).

What is junction (depletion) capacitance?

The capacitance from charge stored across the depletion region, Cj = εA/W. Since reverse bias widens W, the capacitance falls — a voltage-controlled capacitor (varactor).

Is there current in the depletion region?

At equilibrium, essentially no net current — diffusion and drift balance. It has fixed charge but no free carriers, so it behaves like an insulator until bias changes its width.

Conclusion & Key Takeaways

The depletion region is the small carrier-free zone that gives the PN junction — and all of modern electronics — its one-way behaviour.

Carrier-free zone

Fixed ions only.

Barrier Vbi

0.7 V Si, 0.3 V Ge.

Forward → narrows

Diode conducts.

Reverse → widens

Blocks current.

Width W

∝ √(Vbi − V).

Cj = εA/W

Voltage-tunable (varactor).

Continue Learning