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A depth-encoding PET detector inserting glass plate between crystal layers

This study introduces a depth-encoding PET detector inserting a glass plate between the pixilated scintillation crystal layers. The principle of proposed design was that the relative amount of light received by each photosensor would be altered by using the glass plate and this change in the light distribution could generate the pattern diagram of the 2D flood histogram identifying DOI as well as X-Y position of γ-ray interaction. A Monte Carlo simulation was conducted to assess the DOI-PET detector of 4 × 4 array photosensor coupled with 2- layer LSO arrays consisting of 4 × 4 arrays of 3 × 3 × 10 mm3 discrete crystals. The traced light distribution for each event was converted by the modified resistive charge division networks into the 2D flood histogram. Optical glass plates with 11 different thicknesses, ranging from 0 to 10 mm with a 1 mm step, were modeled to estimate the thickness allowing to extract the depth information from the 2D flood histogram. An experimental study was performed to acquire the flood histograms of the DOI-PET detectors with 3 and 5 mm thick glass plate. The effect of glass plate on light loss and count rate loss were assessed for two detector configurations with and without glass plate. The simulation results showed that the flood histogram without overlapping of each crystal position could be generated for the detectors inserting the glass plates with thickness of 3 ∼ 10 mm, which were also demonstrated in the acquired flood histograms obtained by the experimental study. The light and count rate losses measured from DOI-PET detector with 3 mm thick glass plate was ∼5% and ∼2%, respectively. This study demonstrated that the proposed DOI-PET detector could extract the 3D γ-ray interaction position without considerable performance degradations of PET detector from the 2D flood histogram.