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Appendix
ImaGe INteNsIFIeRs
An Image intensifier is an evacuated, proximity-focus device that amplifies the intensity of an incoming signal. The
device is small, typically 1-2 inches in diameter and 1 inch thick. As well as amplifying incoming signal, an image
intensifier can rapidly be switched on and off, allowing it to be used as a very fast optical shutter in the nanosecond time
regime. The image intensifier used in the system can either be of 2nd generation (‘Gen 2’) or 3rd generation (‘Gen 3’).
There are three major elements in an image intensifier :
•
The photocathode
•
The Micro-Channel Plate (MCP)
•
The output Phosphor screen
PHOTOCATHODES AND WINDOWS
The photocathode is coated on the inside surface of an input window, typically made of silica, MgF2, Borosilicate glass
of fibre-optic plate. The input window typically set the lower detection limit, while the photocathode set the upper
detection wavelength.
When an incoming photon strikes the photocathode, a photoelectron may be emitted, depending on the QE of the
photocathode. This photoelectron is drawn across a small gap towards the MCP by an electric field.
‘Gen 2’
refers to multi-alkali based photocathodes that present a wide wavelength coverage from UV up to ~ 900 nm,
with moderate peak QE up to ~25-30%. The lower detection limited is set by the photocathode substrate, typically Silica
of Magnesium Fluoride (MgF2). These photocathode are quite resistive, and require a metallic underlay (full or grid-type)
to achieve nanosecond gating times (at the expense of a few percent QE).
‘Gen 3’
refers to Gallium-Arsenide (GaAs) – based photocathodes. These are typically deposited on glass - which set the
lowest detection limit at ~ 350 nm, and are sensitive up to ~900 nm. They present peak QE up to 50%.
Note:
Please refer to sections 2.5 and 2.6 for further details on image intensifiers options.
Gating
- The voltage on the photocathode in relation to the input of the MCP can be rapidly toggled between 2 levels. If
the voltage of the photocathode is made positive relative to the input of the MCP, then the photoelectrons will not have
sufficient energy to leave the photocathode and the image intensifier will effectively be OFF.
By switching the voltage the intensifier can be turned ON and OFF. This process is referred to as “Gating”. Gating
periods in the nanosecond scale (billionth of a second) can be readily achieved, making the image intensifier, one of the
fastest optical shutters available.