Calculating photodiode current and voltage

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SUMMARY

This discussion focuses on calculating the current and voltage produced by Hamamatsu Si PIN photodiodes. The photodiodes operate primarily as current sources, with their output current being nearly independent of the applied voltage. Three common operational methods are highlighted: reverse biasing for current output proportional to photon count, shunting into low impedance for wide bandwidth applications, and operating in photovoltaic mode with high input impedance. Each method has distinct advantages and applications, particularly in sensitivity and linearity.

PREREQUISITES
  • Understanding of photodiode operation principles
  • Familiarity with Hamamatsu Si PIN photodiode specifications
  • Knowledge of electrical impedance concepts
  • Basic principles of quantum efficiency in photonics
NEXT STEPS
  • Research "Hamamatsu Si PIN photodiode specifications" for detailed performance metrics
  • Learn about "photodiode reverse biasing techniques" for optimal current output
  • Explore "impedance matching in photodiode applications" for improved signal integrity
  • Investigate "photovoltaic mode operation of photodiodes" for applications in low-light conditions
USEFUL FOR

Electronics engineers, optical engineers, and researchers involved in photonics or sensor technology will benefit from this discussion, particularly those working with photodiode applications and performance optimization.

jollett
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Hi I'm pretty new to the forums. I've been searching and can't find anything on this. Can anyone show me how to calculate the current/voltage produced by a photodiode?
 
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Here are the specs for a typical Hamamatsu Si PIN photodiode.

http://jp.hamamatsu.com/resources/products/ssd/pdf/s3590-08_etc_kpin1052e07.pdf

Look up the spectral response for the wavelength you are interested in (see dotted line for 100% quantum efficiency* in plot). PIN photodiodes are essentially current sources, because the current output is nearly independent of the applied voltage. The depletion depth is much larger than the photon absorption length.

* 100% quantum efficiency is 1 photoelectron per incident photon

Bob S
 
People tend to use the diodes in one of the following three ways:

1. Reverse biased and treated as a current source
2. Shunted into a low value impedance (typically 50 ohms)
3. Operated in the "photo-voltaic" mode

This first method is by and far preferred in that it gives you a current that's proportional to the number of photons. With the proper amplifier, this method is typically fairly sensitive and has a fair bandwidth.

The second method is often used for wide bandwidth applications. Most applications involving a 50 ohm load are based on photo diodes going into test equipment and the sensitivity is poor. However, the linearity is still pretty good - voltage is proportional to photons for a reasonable excitation.

The third method involves leaving the photo diode "unloaded." The following instrument or amplifier has a high input impedance and with even a little light, the diode reaches a saturation point where the output voltage is limited. Typically, you can get up to about .6v and it takes progressively more light to make a moderate increase output voltage.
 
Most likely this can only be answered by an "old timer". I am making measurements on an uA709 op amp (metal can). I would like to calculate the frequency rolloff curves (I can measure them). I assume the compensation is via the miller effect. To do the calculations I would need to know the gain of the transistors and the effective resistance seen at the compensation terminals, not including the values I put there. Anyone know those values?

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