Poster - 01: LabPET II Pixelated APD-Based PET Scanner for High-Resolution Preclinical Imaging
Creators
- Lecomte, Roger1
- Arpin, Louis1
- Beaudoin, Jean-François1
- Bergeron, Mélanie1
- Bouchard, Jonathan1
- Bouziri, Haithem1
- Cadorette, Jules1
- Gaudin, Émilie1
- Jürgensen, Nadia1
- Koua, Konin Calliste1
- Trépanier, Pierre-Yves Lauzier1
- Leroux, Jean-Daniel1
- Loignon-Houle, Francis1
- Njejimana, Larissa1
- Paillé, Maxime1
- Paulin, Caroline1
- Pepin, Catherine1
- Pratte, Jean-François1
- Samson, Arnaud1
- Thibaudeau, Christian1
- and others
- 1. Université de Sherbrooke, Université de Sherbrooke, CIMS/CRCHUS, Université de Sherbrooke, Université de Sherbrooke, Université de Sherbrooke, CIMS/CRCHUS, Université de Sherbrooke, Université de Sherbrooke, 3IT, Université de Sherbrooke, Novalgo Inc., Université de Sherbrooke, Université de Sherbrooke, CIMS/CRCHUS, 3IT, Université de Sherbrooke, Université de Sherbrooke, Université de Sherbrooke, Université de Sherbrooke, 3IT, Université de Sherbrooke (Canada)
Description
Purpose: LabPET II is a new generation APD-based PET scanner designed to achieve sub-mm spatial resolution using truly pixelated detectors and highly integrated parallel front-end processing electronics. Methods: The basic element uses a 4×8 array of 1.12×1.12 mm2 Lu1.9Y0.1SiO5:Ce (LYSO) scintillator pixels with one-to-one coupling to a 4×8 pixelated monolithic APD array mounted on a ceramic carrier. Four detector arrays are mounted on a daughter board carrying two flip-chip, 64-channel, mixed-signal, application-specific integrated circuits (ASIC) on the backside interfacing to two detector arrays each. Fully parallel signal processing was implemented in silico by encoding time and energy information using a dual-threshold Time-over-Threshold (ToT) scheme. The self-contained 128-channel detector module was designed as a generic component for ultra-high resolution PET imaging of small to medium-size animals. Results: Energy and timing performance were optimized by carefully setting ToT thresholds to minimize the noise/slope ratio. ToT spectra clearly show resolved 511 keV photopeak and Compton edge with ToT resolution well below 10%. After correction for nonlinear ToT response, energy resolution is typically 24±2% FWHM. Coincidence time resolution between opposing 128-channel modules is below 4 ns FWHM. Initial imaging results demonstrate that 0.8 mm hot spots of a Derenzo phantom can be resolved. Conclusion: A new generation PET scanner featuring truly pixelated detectors was developed and shown to achieve a spatial resolution approaching the physical limit of PET. Future plans are to integrate a small-bore dedicated mouse version of the scanner within a PET/CT platform.
Additional details
Identifiers
- DOI
- 10.1118/1.4961775;
Publishing Information
- Journal Title
- Medical Physics
- Journal Volume
- 43
- Journal Issue
- 8
- Journal Page Range
- vp.
- ISSN
- 0094-2405
- CODEN
- MPHYA6
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 49038623
- Subject category
- S46: INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY; S60: APPLIED LIFE SCIENCES;
- Descriptors DEI
- BIOMEDICAL RADIOGRAPHY; ENERGY RESOLUTION; GENES; HOT SPOTS; KEV RANGE 100-1000; NONLINEAR PROBLEMS; POSITRON COMPUTED TOMOGRAPHY; SPATIAL RESOLUTION; TIME RESOLUTION
- Descriptors DEC
- COMPUTERIZED TOMOGRAPHY; DIAGNOSTIC TECHNIQUES; EMISSION COMPUTED TOMOGRAPHY; ENERGY RANGE; KEV RANGE; MEDICINE; NUCLEAR MEDICINE; RADIOLOGY; RESOLUTION; TIMING PROPERTIES; TOMOGRAPHY
Optional Information
- Notes
- (c) 2016 American Association of Physicists in Medicine