Photonics & optoelectronics

Photodiode

A photodiode runs an LED in reverse: instead of turning current into light, it turns light into current. When a photon with enough energy strikes the semiconductor junction, it knocks an electron loose, creating an electron–hole pair; the diode's built-in field sweeps them apart, and that flow of freed charges is a tiny current proportional to how brightly the light shines. Shine more light, get more current — the device is an honest, linear light meter built from a single diode.

It is usually operated in reverse bias, which widens the depletion region (the 'collecting zone') and speeds the response, so photodiodes can follow light flickering billions of times a second — exactly what a fibre-optic receiver needs to decode laser pulses. Variants trade speed for sensitivity: a PIN diode for fast clean detection, an avalanche photodiode (APD) that multiplies each freed electron into an avalanche for faint-light work, and the humble solar cell, which is just a large photodiode optimised to harvest power rather than read signals.

I_photo = R · P_optical (R = responsivity in A/W)

Don't confuse the two modes: in photovoltaic mode (zero bias) the photodiode generates its own voltage and is low-noise but slow; in photoconductive mode (reverse bias) it's fast but adds dark-current noise — receivers pick speed, light meters pick low noise.

Also called
photodetector光電二極體光偵測器