Photon Counting Energy Dispersive Detector Arrays for X-ray Imaging

被引:245
作者
Iwanczyk, Jan S. [1 ]
Nygard, Einar [1 ,2 ]
Meirav, Oded [3 ]
Arenson, Jerry [3 ]
Barber, William C. [1 ]
Hartsough, Neal E. [1 ]
Malakhov, Nail [1 ,2 ]
Wessel, Jan C. [1 ,2 ]
机构
[1] DxRay Inc, Northridge, CA 91324 USA
[2] Interon AS, Asken, Norway
[3] GE Global Res, Haifa, Israel
基金
美国国家卫生研究院;
关键词
CdTe; CdZnTe; photon counting computed tomography; X-ray detectors; COMPUTED-TOMOGRAPHY; READOUT; CDTE;
D O I
10.1109/TNS.2009.2013709
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
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 (CZT) 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 reduce X-ray dose to the patient. A very high X-ray flux is utilized in many of these applications. For example, CT scanners can produce similar to 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 CZT 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 using discrete electronics and a Co-57 source. An output rate of 6 X 10(6) counts per second per individual pixel has been obtained with our ASIC readout electronics and a clinical CT X-ray tube. Additionally, the first clinical CT images, taken with several of our prototype photon-counting and energy-dispersive detector modules, are shown.
引用
收藏
页码:535 / 542
页数:8
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