{"title":"Evaluation of a lead-loaded plastic scintillator for next-generation positron emission tomography detectors using Geant4 simulation.","authors":"Makoto Yamazaki, Masahiro Sato","doi":"10.1186/s40658-026-00941-w","DOIUrl":null,"url":null,"abstract":"<p><strong>Purpose: </strong>Lead-loaded plastic scintillators are promising candidates for next-generation positron emission tomography (PET) detectors owing to their short fluorescence decay times, high machinability and low production cost. However, their γ-ray detection performance has not been fully quantified. This study evaluated the detection efficiency and energy-resolution characteristics of a 5 wt% lead-loaded plastic scintillator (EJ-256) and compared its performance with that of a conventional polyvinyltoluene (PVT) scintillator.</p><p><strong>Methods: </strong>Monte Carlo simulations were performed using Geant4. Monoenergetic 511 keV gamma rays (100 000 events) were irradiated onto scintillator blocks with thicknesses varied from 20 mm to 200 mm in 5 mm increments. The resulting absorbed-energy spectra were analysed using ROOT to determine detection efficiency and the simulated full width at half maximum (FWHM) of the 511-keV photopeak. To identify the thickness region at which detection efficiency saturated, a non-parametric Kruskal-Wallis test was conducted to consecutive thickness groups to determine the point beyond which differences were no longer statistically significant (p > 0.05).</p><p><strong>Results: </strong>EJ-256 exhibited a distinct 511 keV photopeak, whereas PVT showed only a broad Compton continuum. The detection efficiency increased from 0.9% at 20 mm to 2.9% at 200 mm and saturated above approximately 135 mm, consistent with the Kruskal-Wallis analysis. The simulated 511-keV photopeak width remained stable at approximately 10% FWHM across all thicknesses.</p><p><strong>Conclusion: </strong>These results indicate that EJ-256 demonstrates photon-absorption performance comparable to that of conventional inorganic PET scintillators, while offering substantially faster temporal response and reduced fabrication cost. This combination suggests strong potential for application in future time-of-flight PET detector modules.</p>","PeriodicalId":11559,"journal":{"name":"EJNMMI Physics","volume":"13 1","pages":""},"PeriodicalIF":3.5000,"publicationDate":"2026-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC13620012/pdf/","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"EJNMMI Physics","FirstCategoryId":"3","ListUrlMain":"https://doi.org/10.1186/s40658-026-00941-w","RegionNum":2,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"RADIOLOGY, NUCLEAR MEDICINE & MEDICAL IMAGING","Score":null,"Total":0}
引用次数: 0
Abstract
Purpose: Lead-loaded plastic scintillators are promising candidates for next-generation positron emission tomography (PET) detectors owing to their short fluorescence decay times, high machinability and low production cost. However, their γ-ray detection performance has not been fully quantified. This study evaluated the detection efficiency and energy-resolution characteristics of a 5 wt% lead-loaded plastic scintillator (EJ-256) and compared its performance with that of a conventional polyvinyltoluene (PVT) scintillator.
Methods: Monte Carlo simulations were performed using Geant4. Monoenergetic 511 keV gamma rays (100 000 events) were irradiated onto scintillator blocks with thicknesses varied from 20 mm to 200 mm in 5 mm increments. The resulting absorbed-energy spectra were analysed using ROOT to determine detection efficiency and the simulated full width at half maximum (FWHM) of the 511-keV photopeak. To identify the thickness region at which detection efficiency saturated, a non-parametric Kruskal-Wallis test was conducted to consecutive thickness groups to determine the point beyond which differences were no longer statistically significant (p > 0.05).
Results: EJ-256 exhibited a distinct 511 keV photopeak, whereas PVT showed only a broad Compton continuum. The detection efficiency increased from 0.9% at 20 mm to 2.9% at 200 mm and saturated above approximately 135 mm, consistent with the Kruskal-Wallis analysis. The simulated 511-keV photopeak width remained stable at approximately 10% FWHM across all thicknesses.
Conclusion: These results indicate that EJ-256 demonstrates photon-absorption performance comparable to that of conventional inorganic PET scintillators, while offering substantially faster temporal response and reduced fabrication cost. This combination suggests strong potential for application in future time-of-flight PET detector modules.
期刊介绍:
EJNMMI Physics is an international platform for scientists, users and adopters of nuclear medicine with a particular interest in physics matters. As a companion journal to the European Journal of Nuclear Medicine and Molecular Imaging, this journal has a multi-disciplinary approach and welcomes original materials and studies with a focus on applied physics and mathematics as well as imaging systems engineering and prototyping in nuclear medicine. This includes physics-driven approaches or algorithms supported by physics that foster early clinical adoption of nuclear medicine imaging and therapy.