Photodiode - Reverse Bias Operation

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Discussion Overview

The discussion centers around the operation of photodiodes in reverse bias, particularly their use as light intensity sensors. Participants explore the relationship between light intensity, current output, and the effects of resistance in series with the photodiode, as well as the implications of reverse bias on dark current and sensing bandwidth.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions whether the current through a reverse-biased photodiode is affected by the series resistance, suggesting that the photodiode may act as a constant current source regardless of this resistance.
  • Another participant agrees that the voltage across the series resistor is dependent on the photocurrent and notes that reverse bias improves sensing bandwidth, prompting a question about the mechanism behind this improvement.
  • A participant explains that reverse biasing reduces the 'dark' current, making the current produced more indicative of light presence, although they express uncertainty about the accuracy of their explanation.
  • One participant models the photodiode as a current source with high output impedance, indicating that voltage changes have little effect on current.
  • Another participant mentions that dark current is temperature dependent and caused by thermal hole/electron creation, while also noting the effects of forward biasing on the photodiode's operation.
  • There is a discussion about the specific reasons for reverse biasing photodiodes, with one participant questioning the existence of applications that utilize forward biasing.

Areas of Agreement / Disagreement

Participants express varying views on the effects of reverse bias on dark current and the operational characteristics of photodiodes. There is no consensus on the implications of series resistance or the conditions under which forward biasing might be applicable.

Contextual Notes

Some participants reference the relationship between dark current and temperature, as well as the effects of reverse bias on the depletion region and capacitance, but these points remain unresolved and are contingent on further clarification.

tomizzo
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Hello,

I'm attempting to use a photodiode as a light intensity sensor. However, I have a question regarding the operation of a photodiode in a reverse biased position. The current going through the photodiode is dependent on the light received, and is not affected much by the reverse biased voltage (assuming you're applying reasonable voltages). However, wouldn't the current be dependent on the resistance that is in series with the photodiode? The datasheets I've been reading illustrate the relationship between the light received and the current produced, but there is no mentioning of any resistance. Does this mean that photodiode will act as a constant current source regardless of the resistance used in series with the photodiode?

I've attached an image of the circuit in question.

I appreciate any help!
 

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Pretty much. The voltage across that resistor R is dependent on the photocurrent produced by the diode. The main reason to put the negative voltage bias across a photodiode is to improve the sensing bandwidth. Do you know how the reverse bias improves the sensing bandwidth of the photodiode? :smile:
 
Thanks berkeman! I'm not sure if I know the answer to your question, but I'll give it a shot:

The photodiode will produce a current in the absence of light which is undesired. By reverse biasing the diode, the 'dark' current will be decreased, thus the current that will be produced will be more indicative of the presence of light and will be less skewed by the 'dark' current. Am I in the ballpark?
 
tomizzo said:
Thanks berkeman! I'm not sure if I know the answer to your question, but I'll give it a shot:

The photodiode will produce a current in the absence of light which is undesired. By reverse biasing the diode, the 'dark' current will be decreased, thus the current that will be produced will be more indicative of the presence of light and will be less skewed by the 'dark' current. Am I in the ballpark?

Interesting, I didn't know that about the dark current. Do you have a reference for that so I can refresh my memory? :smile:

As you increase the reverse bias of any diode, what happens to the depletion region width? What effect does that have on changing the capacitance across the junction?
 
The photo diode is modeled as a current source. Current sources have high output impedance (voltage changes make little change in current, so effective internal R must be large).

In addition there is the effect berkeman is referring to that impacts the response time to light (not the accuracy). It is very important and is fundamental to any light sensing application. It is usually enumerated in the datasheet tables.

I'm not sure why you think increasing the voltage would decrease the dark current.
 
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It's my understanding that lacking light a photodiode is just a diode. It should have a tiny reverse bias current (dark current) that is slightly voltage dependent if I remember my VI curve.

I think the dark current is temperature dependent as well. I think it's caused in part by thermal hole/electron creation. Other radiation sources also play a part.

Forward biasing it would usually swamp the photo effect in the forward current. This could be avoided by keeping any forward voltage well below the bias current knee.
 
Jeff, there are very specific reasons why photo diodes are reverse biased. I can't think of any implementations where they would be forward biased in any way (zero bias photo-voltaic mode is common though). Do you have some examples for forward bias?
 
meBigGuy said:
Jeff, there are very specific reasons why photo diodes are reverse biased. I can't think of any implementations where they would be forward biased in any way (zero bias photo-voltaic mode is common though). Do you have some examples for forward bias?
I'm not aware of any applications. But technically it could be done.
 

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