Physical principles
Semiconductor lasers
Article REF: E2660 V1
Physical principles
Semiconductor lasers

Author : Jean-Claude BOULEY

Publication date: August 10, 2007 | Lire en français

Logo Techniques de l'Ingenieur You do not have access to this resource.
Request your free trial access! Free trial

Already subscribed?

2. Physical principles

In the 1960s, once it had been demonstrated that certain semiconductors, such as gallium arsenide (GaAs), could spontaneously emit photons by recombination of electron-hole pairs in a p-n junction, several experimenters observed light amplification by stimulated emission in junctions through which a high current flowed. The threshold of stimulated emission appeared for a quantity of electron-hole pairs satisfying a condition analogous to that of population inversion in atomic systems. Then, following the example of gas lasers, by inserting this amplifying medium into a Fabry-Pérot-type optical cavity, we multiplied light amplification and, in 1962, created the first oscillator, or semiconductor laser, emitting at 0.9 µm.

Since then, diode structures and properties have evolved considerably. This progress has been achieved thanks to the discovery of new semiconductors,...

You do not have access to this resource.
Logo Techniques de l'Ingenieur

Exclusive to subscribers. 97% yet to be discovered!

You do not have access to this resource. Click here to request your free trial access!

Already subscribed?


Article included in this offer

"Optics and photonics"

( 202 articles )

Complete knowledge base

Updated and enriched with articles validated by our scientific committees

Services

A set of exclusive tools to complement the resources

View offer details