Vis Photodiode

A visible-light photodiode generates a current when photons strike its p-n junction. In reverse-bias (photoconductive mode) it responds very fast; with no bias (photovoltaic mode) it produces a small open-circuit voltage. Either way, the current is proportional to illuminance across several decades.

Incident photons with energy above the semiconductor's bandgap create electron-hole pairs in the depletion region. Reverse bias sweeps these carriers apart before they recombine, generating a photocurrent. The response wavelength range is set by the bandgap — silicon peaks at ~800 nm and covers 350–1100 nm.

In plain terms

A tiny solar cell tuned to the visible spectrum: each photon that arrives kicks an electron across the junction, generating a current proportional to light intensity.

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Key specifications

When not to use it

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Where you will find it

A short history

A silicon photodiode relies on the internal photoelectric effect: light with energy exceeding silicon's band gap excites electrons from the valence band into the conduction band, creating electron-hole pairs. In the depletion region, the internal electric field drives electrons toward the N-region and holes toward the P-region, so connecting the diode to a circuit produces a current proportional to incident light, useful for optical sensing.

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