Difference between revisions of "Silicon photomultiplier"

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'''Silicon photomultipliers''' (abbrev. '''SiPM''') are photon-sensitive detectors operating as '''Single-photon avalanche diodes''' ('''SPAD''').
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== Principle of Photodiodes ==
 
== Principle of Photodiodes ==
 
A SiPM detector is formed by a pixelated matrix of photodiodes. Each photodiode consists of a junction of positively and negatively doped silicon ('''p-n junction'''). A depleted region which is devoid of free charge carriers is formed in between the differently doped silicon materials. By applying a reverse-voltage to the photodiodes, the depleted region can be enlarged to extend through the entire sensor.  
 
A SiPM detector is formed by a pixelated matrix of photodiodes. Each photodiode consists of a junction of positively and negatively doped silicon ('''p-n junction'''). A depleted region which is devoid of free charge carriers is formed in between the differently doped silicon materials. By applying a reverse-voltage to the photodiodes, the depleted region can be enlarged to extend through the entire sensor.  
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If the reverse-voltage is high enough to exceed the breakdown voltage of the p-n junction, the diode is said to operate in '''Geiger-mode'''. The energy of a single charge carrier accelerated by the electric field is sufficient to create additional electron-hole pairs which in turn liberate even more charge carriers. Ultimately, the multiplication process can lead to a self-sustaining avalanche.
 
If the reverse-voltage is high enough to exceed the breakdown voltage of the p-n junction, the diode is said to operate in '''Geiger-mode'''. The energy of a single charge carrier accelerated by the electric field is sufficient to create additional electron-hole pairs which in turn liberate even more charge carriers. Ultimately, the multiplication process can lead to a self-sustaining avalanche.
 
 
 
== SiPM Photosensors ==
 
== SiPM Photosensors ==
  
 
When combining a multitude of photodiodes designed and operated as described in the previous sections, a SiPM detector is formed. The size of individual pixels (or diodes) ranges from 10 to 100 micrometres.
 
When combining a multitude of photodiodes designed and operated as described in the previous sections, a SiPM detector is formed. The size of individual pixels (or diodes) ranges from 10 to 100 micrometres.

Latest revision as of 16:59, 4 April 2020

Silicon photomultipliers (abbrev. SiPM) are photon-sensitive detectors operating as Single-photon avalanche diodes (SPAD).


Principle of Photodiodes

A SiPM detector is formed by a pixelated matrix of photodiodes. Each photodiode consists of a junction of positively and negatively doped silicon (p-n junction). A depleted region which is devoid of free charge carriers is formed in between the differently doped silicon materials. By applying a reverse-voltage to the photodiodes, the depleted region can be enlarged to extend through the entire sensor. The passage of ionizing radiation through a photodiode creates electron-hole pairs. These liberated charge carriers are accelerated by the electric field in the depleted region towards the anode (holes) or cathode (electrons).

The Geiger Mode

Current-Voltage characteristic of a diode. A SiPM operates in the Breakdown regime.

If the reverse-voltage is high enough to exceed the breakdown voltage of the p-n junction, the diode is said to operate in Geiger-mode. The energy of a single charge carrier accelerated by the electric field is sufficient to create additional electron-hole pairs which in turn liberate even more charge carriers. Ultimately, the multiplication process can lead to a self-sustaining avalanche.

SiPM Photosensors

When combining a multitude of photodiodes designed and operated as described in the previous sections, a SiPM detector is formed. The size of individual pixels (or diodes) ranges from 10 to 100 micrometres.