In PET detectors based on monolithic scintillators, the photon impact position can be estimated from the light intensity distribution (LD) on the photodetector pixels. Typically, there is a poor estimation of the interaction positions towards the edges when linear algorithms such as Center of Gravity (CoG) are used. We present a novel method to determine the interaction coordinates in thick monolithic crystals filtering the digitized LDs from each gamma-event by means of an autocorrelation filter and the raise to power (RTP) positioning algorithm to reduce the border effects. The experimental setup was based on two detector blocks based on monolithic LYSO scintillator crystals (50x50x20 mm3). Each crystal is coupled to a SiPMs array as 12x12 photosensors and an electronic readout that outputs information of each SiPM row and column. Between the detector blocks, a collimated array of 9x9 22Na sources, separated 5 mm each other, was placed. The optimum power to use in the RTP positioning algorithm was determined using the third order intercept point (IP3) from plots of the measured coordinates versus known positions. After applying the autocorrelation and RTP fifth to the data, we found an improvement of the spatial resolution from 2.5 mm when CoG is used, to 1.2 mm in the crystal center region. In this work we show how to accurately resolve 3D photon impact coordinates in thick monolithic crystals using autocorrelation filters merged with RTP methods. After applying the new approach it is possible to accurately resolve impacts close to the entrance of 20 mm thick LYSO scintillators. The reached spatial resolution at any photon depth of interaction is comparable with state-of-the-art crystal array approaches with the advantage of the proposed work to also provide continuous depth of interaction information.
. 2015 May 18;2(Suppl 1):A5. doi: 10.1186/2197-7364-2-S1-A5
3D photon impact determination in monolithic crystals based on autocorrelation filters and RTP methods
Pablo Conde
1,✉, Antonio Gonzalez
1, Marco Bettiol
2, Andrea Fabbri
2, Roberto Pani
2, José María Benlloch Baviera
1, Albert Talens Aguilar
1, Liczandro Hernandez
1, Filomeno Sanchez
1
Pablo Conde
1Institute for Instrumentation in Molecular Imaging, I3M-CSIC, Valencia, Spain
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Antonio Gonzalez
1Institute for Instrumentation in Molecular Imaging, I3M-CSIC, Valencia, Spain
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Marco Bettiol
2Department of Molecular Medicine, Sapienza University of Rome, Italy
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Andrea Fabbri
2Department of Molecular Medicine, Sapienza University of Rome, Italy
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Roberto Pani
2Department of Molecular Medicine, Sapienza University of Rome, Italy
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José María Benlloch Baviera
1Institute for Instrumentation in Molecular Imaging, I3M-CSIC, Valencia, Spain
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Albert Talens Aguilar
1Institute for Instrumentation in Molecular Imaging, I3M-CSIC, Valencia, Spain
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Liczandro Hernandez
1Institute for Instrumentation in Molecular Imaging, I3M-CSIC, Valencia, Spain
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Filomeno Sanchez
1Institute for Instrumentation in Molecular Imaging, I3M-CSIC, Valencia, Spain
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1Institute for Instrumentation in Molecular Imaging, I3M-CSIC, Valencia, Spain
2Department of Molecular Medicine, Sapienza University of Rome, Italy
✉
Corresponding author.
Conference
PSMR 2015: 4th Conference on PET/MR and SPECT/MR
La Biodola, Isola d'Elba, Italy
17-21 May 2015
Collection date 2015 Dec.
© Conde et al; licensee Springer. 2015
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
PMCID: PMC4798656 PMID: 26956308
