Literature DB >> 23611889

Sub-200 ps CRT in monolithic scintillator PET detectors using digital SiPM arrays and maximum likelihood interaction time estimation.

Herman T van Dam1, Giacomo Borghi, Stefan Seifert, Dennis R Schaart.   

Abstract

Digital silicon photomultiplier (dSiPM) arrays have favorable characteristics for application in monolithic scintillator detectors for time-of-flight positron emission tomography (PET). To fully exploit these benefits, a maximum likelihood interaction time estimation (MLITE) method was developed to derive the time of interaction from the multiple time stamps obtained per scintillation event. MLITE was compared to several deterministic methods. Timing measurements were performed with monolithic scintillator detectors based on novel dSiPM arrays and LSO:Ce,0.2%Ca crystals of 16 × 16 × 10 mm(3), 16 × 16 × 20 mm(3), 24 × 24 × 10 mm(3), and 24 × 24 × 20 mm(3). The best coincidence resolving times (CRTs) for pairs of identical detectors were obtained with MLITE and measured 157 ps, 185 ps, 161 ps, and 184 ps full-width-at-half-maximum (FWHM), respectively. For comparison, a small reference detector, consisting of a 3 × 3 × 5 mm(3) LSO:Ce,0.2%Ca crystal coupled to a single pixel of a dSiPM array, was measured to have a CRT as low as 120 ps FWHM. The results of this work indicate that the influence of the optical transport of the scintillation photons on the timing performance of monolithic scintillator detectors can at least partially be corrected for by utilizing the information contained in the spatio-temporal distribution of the collection of time stamps registered per scintillation event.

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Year:  2013        PMID: 23611889     DOI: 10.1088/0031-9155/58/10/3243

Source DB:  PubMed          Journal:  Phys Med Biol        ISSN: 0031-9155            Impact factor:   3.609


  16 in total

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Authors:  Eric Berg; Simon R Cherry
Journal:  Semin Nucl Med       Date:  2018-03-12       Impact factor: 4.446

2.  Side readout of long scintillation crystal elements with digital SiPM for TOF-DOI PET.

Authors:  Jung Yeol Yeom; Ruud Vinke; Craig S Levin
Journal:  Med Phys       Date:  2014-12       Impact factor: 4.071

3.  Analytical calculation of the lower bound on timing resolution for PET scintillation detectors comprising high-aspect-ratio crystal elements.

Authors:  Joshua W Cates; Ruud Vinke; Craig S Levin
Journal:  Phys Med Biol       Date:  2015-06-17       Impact factor: 3.609

4.  Initial performance studies of a wearable brain positron emission tomography camera based on autonomous thin-film digital Geiger avalanche photodiode arrays.

Authors:  Charles R Schmidtlein; James N Turner; Michael O Thompson; Krishna C Mandal; Ida Häggström; Jiahan Zhang; John L Humm; David H Feiglin; Andrzej Krol
Journal:  J Med Imaging (Bellingham)       Date:  2016-11-22

Review 5.  Update on novel trends in PET/CT technology and its clinical applications.

Authors:  Stephan Walrand; Michel Hesse; François Jamar
Journal:  Br J Radiol       Date:  2016-11-25       Impact factor: 3.039

6.  A multiplexed TOF and DOI capable PET detector using a binary position sensitive network.

Authors:  M F Bieniosek; J W Cates; C S Levin
Journal:  Phys Med Biol       Date:  2016-10-14       Impact factor: 3.609

7.  Total Body PET: Why, How, What for?

Authors:  Suleman Surti; Austin R Pantel; Joel S Karp
Journal:  IEEE Trans Radiat Plasma Med Sci       Date:  2020-04-03

8.  Using convolutional neural networks to estimate time-of-flight from PET detector waveforms.

Authors:  Eric Berg; Simon R Cherry
Journal:  Phys Med Biol       Date:  2018-01-11       Impact factor: 3.609

9.  A large area, silicon photomultiplier-based PET detector module.

Authors:  Rr Raylman; A Stolin; S Majewski; J Proffitt
Journal:  Nucl Instrum Methods Phys Res A       Date:  2014-01-21       Impact factor: 1.455

Review 10.  Advances in time-of-flight PET.

Authors:  Suleman Surti; Joel S Karp
Journal:  Phys Med       Date:  2016-01-06       Impact factor: 2.685

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