Difference between revisions of "SiPM Radiation Hardness Tests"

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# Relaxation time (of duration determined by the apparent healing rate)  with ''full measurement'' performed periodically.
 
# Relaxation time (of duration determined by the apparent healing rate)  with ''full measurement'' performed periodically.
 
# Repetition of 1. and 2. as desired to determine the recovery extent
 
# Repetition of 1. and 2. as desired to determine the recovery extent
 +
# Proceed with a longer irradiation period until significant curvature is seen in the change of the performance parameters in order to measure the decay function (e.g. two exponential?)
 
# Irradiate the unit for a much longer duration - until some saturation of the performance parameters is seen. This will help determine the offset in the model of the deterioration of performance parameters.
 
# Irradiate the unit for a much longer duration - until some saturation of the performance parameters is seen. This will help determine the offset in the model of the deterioration of performance parameters.
  
 +
"Full measurement" above refers to the following:
 +
# collection of an ensemble of pulse integrals in the dark to determine the dark rate and gain
 +
# collection of an ensemble of pulse integrals with a pulser at low setting to determine gain, and photo-detection efficiency
  
 
+
Performing (2) at low enough pulser settings to count photons allows a check of the gain against the result in the dark count analysis. In the worst case, higher intensity light pulses may be used: the efficiency is then determined using the gain determined in (1).
 
 
## periodically acquire an ensemble of pulses in the dark to determine gain, and dark rate
 
## periodically acquire an ensemble of pulses in the with a pulser to determine gain, and photo-detection efficiency
 
  
 
== Links ==
 
== Links ==

Revision as of 06:17, 12 August 2010

Although not discussed in the original requirements of the tagger microscope photo-detection, recent measurements have raised radiation hardness (specifically due to neutrons) as a concern for silicon photomultiplier (SiPM) readout. Radiation tests of Hamamatsu and SensL 3x3mm2 units have been started by Dr. Yi Qiang at Jefferson Lab. A similar test is necessary for the Photonique SiPM's currently intended for outfitting the tagger microscope.

Proposed Tests

Dose Selection

To suggest appropriate dose the following considerations are offered:

  1. since a sensor undergoes annealing (as has already been reported in literature) concurrently with the irradiation, an equilibrium may exist between the two processes or, at the very least, the degradation is slowed.
  2. much higher dose rates are applied in radiation hardness tests since the time scale of these tests is much smaller than the lifetime of the equipment in the Hall D complex

For these reasons, attempting to match the radiation dose of some nominal lifetime of the equipment based on some nominal neutron background is not important. Instead, a proper measurement of the damage rate, based on the separate performance parameters: dark rate, photo-detection efficiency and gain, as well as the healing rate of these parameters will offer a model for estimating the lifetime of these devices in their intended role. Therefore, doses should be selected roughly based on how much it takes to demonstrate a change in these performance parameters.

Since:

  1. dose rate is quoted per mass irradiated
  2. the mass of the silicon medium in a SiPM scales with the area (width of the wafers, for our purposes, taken to be roughly the same between various SiPMs)
  3. dark rate (current) scales with the area of the wafer

it seems therefore that similar doses should be applied to the Photonique SiPM as have been found effective in measurements with Hamamatsu and SensL units.


Proposed Measurement Program

  1. Irradiation with about 40 rem over the course of a few days (source strength selected appropriately) with full measurement performed periodically.
  2. Relaxation time (of duration determined by the apparent healing rate) with full measurement performed periodically.
  3. Repetition of 1. and 2. as desired to determine the recovery extent
  4. Proceed with a longer irradiation period until significant curvature is seen in the change of the performance parameters in order to measure the decay function (e.g. two exponential?)
  5. Irradiate the unit for a much longer duration - until some saturation of the performance parameters is seen. This will help determine the offset in the model of the deterioration of performance parameters.

"Full measurement" above refers to the following:

  1. collection of an ensemble of pulse integrals in the dark to determine the dark rate and gain
  2. collection of an ensemble of pulse integrals with a pulser at low setting to determine gain, and photo-detection efficiency

Performing (2) at low enough pulser settings to count photons allows a check of the gain against the result in the dark count analysis. In the worst case, higher intensity light pulses may be used: the efficiency is then determined using the gain determined in (1).

Links