Photon counting energy dispersive detector arrays for x-ray imaging

The development of an innovative detector technology for photon counting in X-ray imaging is reported. This new generation of detectors, based on pixellated cadmium telluride (CdTe) and cadmium zinc telluride (CdZnTe) detector arrays electrically connected to application specific integrated circuits...

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Hauptverfasser: Iwanczyk, J.S., Nygard, E., Meirav, O., Arenson, J., Barber, W.C., Hartsough, N.E., Malakhov, N., Wessel, J.C.
Format: Tagungsbericht
Sprache:eng
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Zusammenfassung:The development of an innovative detector technology for photon counting in X-ray imaging is reported. This new generation of detectors, based on pixellated cadmium telluride (CdTe) and cadmium zinc telluride (CdZnTe) detector arrays electrically connected to application specific integrated circuits (ASICs) for readout, will produce fast and highly efficient photon counting and energy dispersive x-ray imaging. There are a number of applications that can greatly benefit from these novel imagers including mammography, planar radiography, and computed tomography (CT). Systems based on this new detector technology can provide compositional analysis of tissue through spectroscopic x-ray imaging, significantly improve overall image quality, and may significantly reduced x-ray dose to the patient. Very high x-ray flux are utilized in many of these applications. For example, CT scanners can produce ~100 Mphotons/mm 2 /s in the unattenuated beam. High flux is required in order to collect sufficient photon statistics in the measurement of the transmitted flux (attenuated beam) during the very short time frame of a CT scan. This high count rate combined with a need for high detection efficiency requires the development of detector structures that can provide a response signal much faster than the transit time of carriers over the whole detector thickness. We have developed CdTe and CdZnTe detector array structures which are 3 mm thick with 16 x 16 pixels and a 1 mm pixel pitch. These structures, in the two different implementations presented here, utilize either a small pixel effect or a drift phenomenon. An energy resolution of 4.75% at 122 keV has been obtained with a 30 ns peaking time. An output rate of 6 x 10 6 counts per second per individual pixel has been obtained with ASIC readout electronics. Additionally, the first clinical CT images, taken with several of our prototype photon counting and energy dispersive detector modules, are shown.
ISSN:1082-3654
2577-0829
DOI:10.1109/NSSMIC.2007.4436710