2013
DOI: 10.1016/j.nima.2013.07.054
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Synchrotron characterisation of non-uniformities in a small pixel cadmium zinc telluride imaging detector

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Cited by 11 publications
(11 citation statements)
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“…The spectroscopic performance of the HF-CdZnTe detector compares favourably to the performance achieved using spectroscopic-grade CdZnTe from Redlen technologies [ 47 ], also coupled with the HEXITEC ASIC in a detector of 2 mm thickness and 250 pixel pitch. Using the spectroscopic-grade CdZnTe, the average FWHM of the 59.5 keV photopeak for the entire detector was 1.74 ± 0.39 keV for isolated events only, compared with 0.95 ± 0.07 keV achieved with the HF-CdZnTe detector here.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The spectroscopic performance of the HF-CdZnTe detector compares favourably to the performance achieved using spectroscopic-grade CdZnTe from Redlen technologies [ 47 ], also coupled with the HEXITEC ASIC in a detector of 2 mm thickness and 250 pixel pitch. Using the spectroscopic-grade CdZnTe, the average FWHM of the 59.5 keV photopeak for the entire detector was 1.74 ± 0.39 keV for isolated events only, compared with 0.95 ± 0.07 keV achieved with the HF-CdZnTe detector here.…”
Section: Discussionmentioning
confidence: 99%
“…Using the spectroscopic-grade CdZnTe, the average FWHM of the 59.5 keV photopeak for the entire detector was 1.74 ± 0.39 keV for isolated events only, compared with 0.95 ± 0.07 keV achieved with the HF-CdZnTe detector here. Veale et al [ 47 ] showed evidence of local variations in the electric field, linked to the build up of space charge due to carrier trapping and the use of blocking contacts [ 48 ], which would damage spectroscopic performance. The agreement between the experimentally determined charge sharing rates and simulation set to the applied external bias of −750 V ( Figure 9 ), suggests that the electric field strength within the HF-CdZnTe does not significantly suffer from local distortions and is uniform.…”
Section: Discussionmentioning
confidence: 99%
“…While the current iteration of the detector system is now in use at beam lines, a roadmap for STFC's continued development of this technology is in place. In the short term, the aim is to improve the efficiency of the system at energies > 150 keV through the use of thick cadmium zinc telluride sensor material [18] without compromising on the spectroscopic performance of the system. In the longer term, a new generation of the technology will be developed that delivers spectroscopic imaging at frame rates of up to 1 MHz which will meet the needs of future diffraction limited storage ring synchrotrons.…”
Section: Discussionmentioning
confidence: 99%
“…It is also worth noting that there is very little spatial variation in the charge sharing percentage across the entire detector, see Figure 5a, with only major variations observed at the physical edge of the sensor. The spatial uniformity of the charge sharing suggests that the electric field across the detector is also very uniform and does not contain the electric field variations that have been observed previously in spectroscopic-grade CdZnTe material from Redlen [23]. As the HEXITEC system records each frame of data, any charge sharing corrections are applied during data processing, allowing different algorithms to be used.…”
Section: Charge Sharingmentioning
confidence: 99%