a semiconductor diode characterized by unidirectional photoconductivity when exposed to optical radiation. A photodiode is a semiconductor crystal that usually has p-n junction with two metal terminals—one from the p-region and the other from the n-region—and is enclosed in a metal or plastic housing. Photodiodes are made of such materials as Ge, Si, GaAs, or HgCdTe.
A photodiode may operate in either of two modes. In the first mode, the external circuit contains a DC source, thus producing a reverse bias across the p-n junction (see Figure 1); in the second mode, when no DC source is present, a photodiode functions as a valve. When operating in the first mode, a photodiode is used as a photoconductive cell to control the electric current in a circuit in accordance with the variation in the intensity of the incident radiation. The minority carriers produced upon exposure to radiation diffuse through the p-n junction and weaken the junction’s electric field. Over a wide range, the photoelectric current is linearly related to the intensity of the incident radiation and is practically independent of the bias voltage. As a valve, a photodiode—like a semiconductor photocell—is used to generate a photoelectromotive force.
The main parameters of a photodiode are as follows: (1) the threshold sensitivity—that is, the minimum signal detected by a photodiode per unit operating-frequency band—which may be as low as 10–14 watt/hertz½ (W/Hz½); (2) the noise level, which does not exceed 10–9 ampere (A); (3) the spectral sensitivity region, which lies in the range 0.3–15 micrometers; (4) the spectral sensitivity—that is, the ratio of the photoelectric current to the flux of incident monochromatic radiation with a known wavelength-—which is 0.5–1 A/W; and (5) the rise time—that is, the time required to reach a rated value of a photoelectric current—which is of the order of 10–7–10–8 sec.
In an avalanche photodiode, which is a p-n variety, the sensitivity is increased by using the avalanche effect in the p-n junction; the effect is based on the impact ionization of atoms in the junction region by photoelectrons. The avalanche effect multiplies the charge carriers by a factor of 102–104.
Photodiodes with a p-i-n structure are also used. Such photo-diodes have characteristics similar to those of p-n photodiodes, but their rise time is substantially smaller—as low as 10–10 sec.
Photodiodes are used, for example, in automated devices, laser technology, computer technology, and measurement technology.
I. F. USOLTSEV