An avalanche photodiode is a silicon-based semiconductor containing a pn junction consisting of a positively doped p region and a negatively doped n region sandwiching an area of neutral charge termed the depletion region. These diodes provide gain by the generation of electron-hole pairs from an energetic electron that creates an "avalanche" of electrons in the substrate.

The tutorial initializes with both the Photon Intensity and the Reverse Bias sliders set to an arbitrary mid-range value. Photons (yellow) entering the diode first pass through the silicon dioxide layer and then through the n and p layers before entering the depletion region where they excite free electrons (red) and holes (blue), which then migrate to the cathode and anode, respectively. Use the sliders to control the number of photons entering the diode and the reverse bias, which determines the number of electron/hole pairs generated by the photons.

When a semiconductor diode has a reverse bias (voltage) applied and the crystal junction between the p and n layers is illuminated, then a current will flow in proportion to the number of photons incident upon the junction. Avalanche diodes are very similar in design to the silicon p-i-n diode, however the depletion layer in an avalanche photodiode is relatively thin, resulting in a very steep localized electrical field across the narrow junction. In operation, very high reverse-bias voltages (up to 2500 volts) are applied across the device. As the bias voltage is increased, electrons generated in the p layer continue to increase in energy as they undergo multiple collisions with the crystalline silicon lattice. This "avalanche" of electrons eventually results in electron multiplication that is analogous to the process occurring in one of the dynodes of a photomultiplier tube.

Avalanche photodiodes are capable of modest gain (500-1000), but exhibit substantial dark current, which increases markedly as the bias voltage is increased (see Figure 1). They are compact and immune to magnetic fields, require low currents, are difficult to overload, and have a high quantum efficiency that can reach 90 percent. Avalanche photodiodes are now being used in place of photomultiplier tubes for many low-light-level applications.

---

BACK TO DIGITAL IMAGING IN OPTICAL MICROSCOPY

Questions or comments? Send us an email.

© 1998-2022 by Michael W. Davidson and The Florida State University. All Rights Reserved. No images, graphics, scripts, or applets may be reproduced or used in any manner without permission from the copyright holders. Use of this website means you agree to all of the Legal Terms and Conditions set forth by the owners.

This website is maintained by our
Graphics & Web Programming Team
in collaboration with Optical Microscopy at the
National High Magnetic Field Laboratory.

Last modification: Thursday, Feb 11, 2016 at 10:54 AM

Access Count Since July 26, 2000: 72276

Visit the websites of our partners in digital imaging education: