For more optimal dose efficiency, detectors should have as much active area capturing photons as possible. In conventional EIDs, light in one detector pixel can scatter into a neighboring pixel, a phenomenon called optical crosstalk that reduces spatial resolution. Because of this, EIDs require a reflector of finite thickness between the scintillator pixels to prevent crosstalk. However, the presence of this reflector reduces the active area of the detector and, thus, its dose efficiency, especially for small-sized detector pixels. Because PCCT doesn’t use a scintillator, there is no need for reflective material between detector pixels. This greatly improves the dose efficiency of the detector, allowing for smaller detector pixel sizes without dose penalty.
PCCT also overcomes a major disadvantage of EID: electronic noise. An EID’s electronic noise is unavoidably combined with true signal into the detector output. When the number of photons is low, electronic noise becomes dominant, degrading image quality. With PCCT, electronic noise from the detector registers below the threshold of lowest energy bin and is thus discarded. In this way, PCCT effectively eliminates electronic noise, which improves image quality.