DocumentCode :
3356727
Title :
An investigation of Lu1.8Gd0.2SiO5:Ce (LGSO) phoswich crystal identification by digital methods
Author :
Bergeron, Mélanie ; Pepin, Catherine M. ; Clerk-Lamalice, Julien ; Thibaudeau, Christian ; Fontaine, Réjean ; Lecomte, Roger
Author_Institution :
Dept. of Nucl. Med. & Radiobiol., Univ. de Sherbrooke, Sherbrooke, QC, Canada
fYear :
2011
fDate :
23-29 Oct. 2011
Firstpage :
1624
Lastpage :
1626
Abstract :
LGSO-90%Lu scintillators are promising new candidates for future positron emission tomography (PET) scanners, offering high light output (90-120% of NaI(Tl) with avalanche photodiode readout) and a range of decay times from τ = 28 ns to τ = 48 ns by varying cerium concentration during the crystal fabrication process. Such diversity of crystal properties makes it possible to create multiple phoswich detector combinations for improving spatial resolution or measuring depth-of-interaction in PET imaging. This investigation was performed to identify the allowable range of decay time differences that can be used in phoswich detector pairs while still achieving acceptable crystal identification accuracy. The various phoswich arrangements were tested using the LabPET digital electronics implemented with different pulse-shape identification algorithms, including least-mean-square (LMS) auto-regressive method and Wiener filter linear optimization method, to obtain the discrimination error rate. Each phoswich pair was tested with three different low-energy thresholds (150, 250 and 350 keV) to help underlining possible limitations. Overall, the Wiener filter yielded better results. As expected, discrimination was more accurate when using the higher energy threshold of 350 keV. Given an arbitrarily chosen maximum identification error rate of 10%, a decay time difference larger than 12 ns was required with the LMS filter and a 250 keV energy threshold. An even larger decay time difference was required if the slowest crystal decay time was greater than 45 ns. With the Wiener filter and a 250 keV threshold, a decay time difference of only 5 ns was found acceptable if the slowest crystal decay time was under 38 ns. In contrast, when the fastest crystal decay time was higher than 38 ns, a decay time difference of 10 ns or more was required. In summary, when using a Wiener filter-based identification algorithm, a relatively wide range of LGSO crystal combinations can- be used to achieve accurate crystal identification in phoswich detectors for PET imaging.
Keywords :
Wiener filters; avalanche photodiodes; cerium; gadolinium compounds; least mean squares methods; lutetium compounds; optimisation; positron emission tomography; pulse shaping; readout electronics; silicon compounds; solid scintillation detectors; LGSO crystal combinations; LMS filter; LabPET digital electronics; Lu1.8Gd0.2SiO5:Ce; Nal(Tl); PET imaging; PET scanners; Wiener filter linear optimization method; Wiener filter-based identification; avalanche photodiode readout; cerium concentration; crystal decay time; crystal fabrication process; crystal properties; depth-of-interaction; digital method; electron volt energy 150 keV; electron volt energy 250 keV; electron volt energy 350 keV; least-mean-square autoregressive method; multiple phoswich detector; phoswich crystal identification; positron emission tomography; pulse-shape identification algorithms; time 28 ns to 48 ns; Least squares approximation;
fLanguage :
English
Publisher :
ieee
Conference_Titel :
Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC), 2011 IEEE
Conference_Location :
Valencia
ISSN :
1082-3654
Print_ISBN :
978-1-4673-0118-3
Type :
conf
DOI :
10.1109/NSSMIC.2011.6154647
Filename :
6154647
Link To Document :
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