TY - GEN
T1 - Studies of CZT for PET applications
AU - Vaska, P.
AU - Bolotnikov, A.
AU - Carini, G.
AU - Camarda, G.
AU - Pratte, J. F.
AU - Dilmanian, F. A.
AU - Park, S. J.
AU - James, R. B.
PY - 2005
Y1 - 2005
N2 - CdZnTe (CZT) has been investigated by several researchers as a detector material for positron emission tomography (PET) applications. CZT detectors can be manufactured into 1 cm3 or larger detectors with pixelated anodes, providing high spatial resolution at the 1 mm level or smaller. Indeed the spatial and energy resolution of CZT can be far superior to those of current state-of-the-art PET detectors, most of which are scintillator-based. On the other hand, at 511 keV its timing performance and photopeak detection efficiency are generally inferior, which pose challenges that must be surmounted. In order to obtain sufficient efficiency with a practical number of electronics channels and interconnections in a realistic full-scale system, the focus is on thick detectors (∼10 mm). However, the timing becomes more challenging with increasing thickness due to the low charge mobility. We evaluated planar and coplanar grid CZT detectors, as well as position-sensitive pixel-anode detectors to assess methods of improving timing performance. For a 7.5-mm thick coplanar grid detector at 1000 V bias, we obtained a preliminary time resolution vs. BaF2 detector of 21 ns FWHM by fitting the digitally sampled rising edge of the cathode signal. Optimization of the front-end electronics and data-processing methods is expected to further improve these results. We are currently characterizing the performance of a pixel cube detector of ∼1 cm3 in size with a single cathode and a 4 × 4 array of anodes with 2.5-mm pitch on the opposing side, for which a data acquisition system has been designed and fabricated.
AB - CdZnTe (CZT) has been investigated by several researchers as a detector material for positron emission tomography (PET) applications. CZT detectors can be manufactured into 1 cm3 or larger detectors with pixelated anodes, providing high spatial resolution at the 1 mm level or smaller. Indeed the spatial and energy resolution of CZT can be far superior to those of current state-of-the-art PET detectors, most of which are scintillator-based. On the other hand, at 511 keV its timing performance and photopeak detection efficiency are generally inferior, which pose challenges that must be surmounted. In order to obtain sufficient efficiency with a practical number of electronics channels and interconnections in a realistic full-scale system, the focus is on thick detectors (∼10 mm). However, the timing becomes more challenging with increasing thickness due to the low charge mobility. We evaluated planar and coplanar grid CZT detectors, as well as position-sensitive pixel-anode detectors to assess methods of improving timing performance. For a 7.5-mm thick coplanar grid detector at 1000 V bias, we obtained a preliminary time resolution vs. BaF2 detector of 21 ns FWHM by fitting the digitally sampled rising edge of the cathode signal. Optimization of the front-end electronics and data-processing methods is expected to further improve these results. We are currently characterizing the performance of a pixel cube detector of ∼1 cm3 in size with a single cathode and a 4 × 4 array of anodes with 2.5-mm pitch on the opposing side, for which a data acquisition system has been designed and fabricated.
UR - https://www.scopus.com/pages/publications/33846574364
U2 - 10.1109/NSSMIC.2005.1596916
DO - 10.1109/NSSMIC.2005.1596916
M3 - Conference contribution
SN - 0780392213
SN - 9780780392212
T3 - IEEE Nuclear Science Symposium Conference Record
SP - 2799
EP - 2802
BT - 2005 IEEE Nuclear Science Symposium Conference Record -Nuclear Science Symposium and Medical Imaging Conference
T2 - Nuclear Science Symposium Conference Record, 2005 IEEE
Y2 - 23 October 2005 through 29 October 2005
ER -