Metascintillators: New Results for TOF-PET Applications

We report on the progress on a first generation of realistic size metascintillators for time-of-flight PET. These heterostructures combine dense LYSO or BGO plates, interleaved with fast scintillator layers producing a bunch of prompt photons from the energy leakage of the recoil photoelectric elect...

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Detalles Bibliográficos
Autores: Lecoq, P., Konstantinou, Georgios, Latella, Riccardo, Moliner, Laura, Nuyts, Johan, Zhang, Lei, Barrio Toala, J., Benlloch Baviera, José María, González Martínez, Antonio Javier
Tipo de recurso: artículo
Estado:Versión aceptada para publicación
Fecha de publicación:2022
País:España
Institución:Consejo Superior de Investigaciones Científicas (CSIC)
Repositorio:DIGITAL.CSIC. Repositorio Institucional del CSIC
OAI Identifier:oai:digital.csic.es:10261/420037
Acceso en línea:http://hdl.handle.net/10261/420037
https://api.elsevier.com/content/abstract/scopus_id/85127068570
Access Level:acceso abierto
Palabra clave:Scintillators
Geometry
Timing
Signal to noise ratio
Crystals
Image reconstruction
Sensitivity
Heterostructure
Metascintillator
Positron emission tomography (PET)
Time of flight (TOF)
Descripción
Sumario:We report on the progress on a first generation of realistic size metascintillators for time-of-flight PET. These heterostructures combine dense LYSO or BGO plates, interleaved with fast scintillator layers producing a bunch of prompt photons from the energy leakage of the recoil photoelectric electron. From a Geant4 simulation of the energy sharing distribution between the dense and the fast scintillator on 42 LYSO-based and 42 BGO-based configurations, a detailed study of the timing performance has been performed on a selection of the most promising 12 LYSO-based and 14 BGO-based metascintillators. A Monte Carlo simulation was first performed to extrapolate from direct measurements of the performance of the metascintillator components, the detector time resolution (DTR), and sensitivity on the basis of the simulated amount of energy leakage to the fast scintillator. An analytic algorithm was then applied to determine an equivalent coincidence time resolution (CTR) from the random association of the DTR distributions from two metapixels in coincidence. This equivalent CTR is calculated in order to obtain the same variance in the reconstructed image as the combination of the DTR distributions of 2 metapixels. Preliminary results confirm that with these simple and still nonoptimized configurations, an equivalent CTR of 150 ps for BGO-based and 140 ps for LYSO-based metapixels of realistic size can be obtained.