Detector of thirds generation
scanner use either high pressure inert gas (usually xenon) or solid state scintillates
coupled with photo bodies. The operating principle of xenon detector is illustrated
on the picture. The detector is constructed with May thin tungsten plates
inside a high pressure xenon chamber. Every other plate is connected to a high
voltage dc supply. For example on GD 8800 detector, the plate connected to 500
v. The remaining plates are electricity floating ans are at approximately 0 V.
A pair of low –high voltage plates forms a single detector cell. When x ray
photon strikes a cell, it causes ionization of xenon gas in a photoelectric
interaction. The interaction release energetic photo electrons to ionize more
ion gas ions. The ionized gas xenon nuclei are collected by the o V plates and
free electrons are collected by positive biased plated (500 V) to produce current
signal. The bias voltage across the plates it set high enough such that are ion
collected rapidly by plates with little recombination of positive and negative
ions in the gas. At the some time, the bias voltage is below the point of the avalanche effect, where a nonlinear magnification of signal occurs. Improperly
biased region, the amount of ionization is linearly proportional to the total
energy of the absorbed x ray photons.
Solid detectors overcome many of
the shortcomings of the xenon detector. The detector is made of small blocks of
scintillating materially, such as CdWO4, Gd2O2S or HiLight, coated with reflective
material and coupled to set of photodiodes.
The light photon produced by the
scintillation process travel in all directions. The scintillatator is coated
with highly reflective material to direct the light toward the photodiodes at
the bottom of the detector. Because of the reflection and absorption in the
scintillator , only small percentage of the light photon reaches the photodiodes
to produce electrical signals.
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