Characterization of CdTe and CdZnTe detectors for gamma-ray imaging applications

被引:65
作者
Verger, L [1 ]
Boitel, M [1 ]
Gentet, MC [1 ]
Hamelin, R [1 ]
Mestais, C [1 ]
Mongellaz, F [1 ]
Rustique, J [1 ]
Sanchez, G [1 ]
机构
[1] CEA, GRE, LETI, Grenoble 9, France
关键词
gamma camera detector; CdTe; CdZnTe; energy resolution; detection efficiency; bi-parametric spectrum; pulse height; rise time; scatter rejection; THM; HPBM; VBM; HBM; TOF; transport properties; mobility; lifetime;
D O I
10.1016/S0168-9002(00)00874-3
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
CEA-LETI in association with Bicron and Crismatec has been developing solid-state gamma camera technology based on CZT. The project included gamma camera head systems development including front-end electronics with an integrated circuit (ASIC), material growth, and detector fabrication and characterization. One feature of the work is the use of linear correlation between the amplitude and the fast rise time of the signal - which corresponds to the electron transit time in the detector, a development that was reported previously and which allows more than 80% of the 122 keV gamma -photons incident on HPBM material to be recovered in a +/- 6.5% 2D window. In the current work, we summarize other methods to improve CZT detector performance and compare them with the Bi-Parametric Spectrum (BPS) method. The BPS method can also be applied as a diagnositic. BPS curve shapes an shown to vary with electric field, and with electron transport properties, and the correction algorithims are seen to be robust over a range of values. In addition, the technique is found to improve detectors from a variety of sources including some with special electrode geometries. In all cases, the BPS method improves efficiency ( > 75%)without degrading energy resolution( +/- 6.5% 2D window) even for a monolithic detector. The method does nut overcome bulk inhomogeneity nor noise which comes from low resistivity. (C) 2001 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:297 / 309
页数:13
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