written 8.4 years ago by
teamques10
★ 68k
|
•
modified 8.4 years ago
|
The photo-diode is in fact a p-n junction put to the exact opposite use as the LED
The variation in current is a function of the incident light
Use of the stimulated absorption of light by the semiconductor material for the generation of electron-hole pairs.
The energy of the absorbed photons to transfer the electrons from the ground to the excited state contributes to the variation in circuit current.
The energy of the absorbed photon must at least be equal to the band-gap of the material for the material to respond to the incoming photons.
PIN diode
A simple way to increase the depletion-region width is to insert a layer of undoped (or lightly doped) semiconductor material between the p–n junction.
Since the middle layer consists of nearly intrinsic material, such a structure is referred to as the p–i–n photodiode.
When photon enters photodetector, the low band gap absorption layer absorbs the photon, and an electron-hole pair is generated. This electron hole pair is called photocarrier.
These photocarriers, under the influence of a strong electric field generated by a reverse bias potential difference across the device as shown in figure produce photocurrent proportional to number of incident photons.
Avalanche Photo Diode (APD)
All detectors require a certain minimum current to operate reliably. The current requirement translates into a minimum power requirement through $P_{in}= \frac{I_p}R$.
Detectors with a large responsivity R are preferred since they require less optical power.
The responsivity of p–i–n photodiodes is limited while Avalanche photodiode (APDs) can have much larger values of R.
Sr no. |
PIN diode |
APD (Avalanche photodiode) |
1 |
PIN does not have high intensity electric field region. |
APD has high intensity electric field region. |
2 |
Photo current ($I_p$) generated is less compared to APD $I_p=qN_\theta$,q = electron charge,= carrier number |
Photo current ($I_p$) generated is more compared to PIN, $I_p=qN_\theta.M$ q = electron charge,$N_\theta$= carrier number,M = multiplication factor |
3 |
Responsivity of PIN is limited. |
Responsivity of APD can have much larger values. |
4 |
They exhibit lower noise levels. |
They exhibit higher noise levels as compared to PIN due to impact ionization and photocurrent multiplication. |
5 |
Response time of PIN is half that of APD. |
Response time of APD is almost double that of PIN. |