New radiation detector technologies for medical imaging, Simulation and modeling of medical imaging system, Multi-modality imaging systems including applicationss
Session chair:
Schulz, Volkmar, (RWTH Aachen University, Institute of Imaging and Computer Vision and Imaging, Aachen, Germany); Efthimiou, Nikos, Dr. (UMCG, Department of Nuclear Medicine, Groningen, Netherlands)
Shortcut:
M-LT-04
Date:
Thursday, 12 November, 2026, 12:45 -
13:05
Location:
MANUEL DE FALLA
Session type:
MIC Session
Contents
Click on an contribution to preview the abstract content.
The underlined authors are the presenters. The authors in bold are the main authors.
12:45
M-LT-04-01
Development of a PET/MRI Compatible Fluorescence Microscope for Simultaneous Cell Tracking in a Small Animal PET/MRI Scanner (#2535)
P. Renn1, J. Schäfers1, N. Jurisa1, C. Pilger2, T. Huser2, K. Schäfers1
1 University of Münster, European Institute for Molecular Imaging, 48149, North Rhine-Westphalia, Germany 2 Bielefeld University, Biomolecular Photonics Research Group, Department of Physics, 33615, North Rhine-Westphalia, Germany
Abstract
Cell tracking in vivo is a key challenge in translational medicine. Positron emission tomography (PET) and magnetic resonance imaging (MRI) offer complementary strengths for this task, yet the validation of tracking algorithms against a reliable ground truth remains unresolved. Fluorescence microscopy can fulfill this role, but its integration into the highly constrained PET/MRI environment poses significant technical challenges. Here, we present a fluorescence microscope (FM) designed for simultaneous operation inside a small-animal PET/MRI scanner, with all custom structural and housing components 3D printed in polylactic acid (PLA). The assembled instrument has a total length of 95 cm and fits within the 35 mm PET insert bore, accommodating sample diameters of up to 21 mm. The imaging probe is rotated via a non-ferromagnetic, friction-driven mechanism, enabling multi-angle acquisition without repositioning the sample, and reliable rotation over the full 360° range was demonstrated under manual control. The system follows an epi-fluorescence configuration with 10× magnification, an excitation wavelength of 488 nm, and a 500 nm longpass filter in the detection path. Characterization with a calibration slide and a Convallaria majalis test specimen yielded a pixel pitch of 0.144 μm/pixel (6.96 pixels/μm), a spatial resolution of 2.32 μm (FWHM), a signal-to-noise ratio (SNR) of 7.21, and a field of view (FoV) of 0.55 × 0.31 mm2 (3816 × 2160 pixels), sufficient to resolve individual cells. These results establish the feasibility of integrating fluorescence microscopy into a PET/MRI scanner and provide the basis for future multimodal cell tracking studies with a reliable optical ground truth.
AcknowledgmentThis work was funded by the Deutsche Forschungsgemeinschaft (DFG) – CRC 1450 – 431460824.
References [1] Wapler, MC, Testud, F, Hucker, P, Leupold, J, v. Elverfeldt, D, Zaitsev, M & Wallrabe, U 2021, ‘MR-compatible optical microscope for in-situ dual-mode MR-optical microscopy’, PLOS ONE, vol. 16, no. 5, p. e0250903: PLOS. [2] Cui, M, Zhou, Y, Wei, B, Zhu, X-H, Zhu, W, Sanders, MA, Ugurbil, K & Chen, W 2017, ‘A proof-of-concept study for developing integrated two-photon microscopic and magnetic resonance imaging modality at ultra-high field of 16.4 tesla’, Scientific Reports, vol. 7, no. 1, p. 2733: Nature Publishing Group. [3] Zhu, X, Li, R, Li, H, Gu, L, Chen, L, Xu, J, Chen, J, Li, Y, Rudin, M, Thompson, G, Zhou, N & Ren, W 2026, ‘MR-Scope: a multi-scale and simultaneous MRI-miniaturized microscopy system for elucidating neurovascular coupling’: bioRxiv. [4] Li, C, Yang, Y, Mitchell, GS & Cherry, SR 2011, ‘Simultaneous PET and multispectral 3-dimensional fluorescence optical tomography imaging system’, Journal of Nuclear Medicine: Official Publication, Society of Nuclear Medicine, vol. 52, no. 8, pp. 1268–1275: Society of Nuclear Medicine.
Hybrid PGI-PET Imaging for Ion-Range Monitoring in Hadron Therapy (#2044)
J. Balibrea Correa1, V. Babiano-Suárez1, J. Lerendegui-Marco1, P. Torres-Sánchez1, I. Ladarescu1, C. Domingo-Pardo1, A. Tarifeño-Saldivia1, M. Pallás2, B. Brusasco2, J. Wulff3, C. Baümer3, S. Rossomme4, A. Warnier4
1 Instituto de Física Corpuscular (CSIC-University of Valencia), Física Nuclear Experimental, Valencia, Spain 2 Universitat Politècnica de Catalunya, Física Nuclear, Barcelona, Spain 3 West German Proton Therapy Centre, Essen, Germany 4 Ion Beam Applications, Louvain, Belgium
Abstract
Hadron therapy is a highly conformal cancer treatment technique that enables superior dose delivery to the tumor while sparing surrounding healthy tissues. However, its full clinical benefit is still limited by uncertainties in proton range within tissue, mainly due to the indirect estimation of ion stopping power from X-ray CT images. These uncertainties lead to safety margins that reduce treatment precision. Real-time, high-accuracy ion-range verification is essential to improve dose delivery and further enhance the therapeutic potential of proton therapy. Among the available approaches, PGI and PET are regarded as the most promising, as they provide complementary information. PGI offers direct correlation with the Bragg peak during irradiation, whereas PET yields high-resolution activity distributions from beta+ emitters produced along the proton path.
In this work, we report recent developments and experimental results obtained with a hybrid PGI-PET system for in situ proton range verification. The system is based on four high-efficiency two-plane Compton imagers arranged in a cross configuration, specifically optimized to enhance PGI sensitivity at the expense of a reduced PET field of view. Experimental campaigns were carried out at commercial IBA Proteus Plus and Proteus One proton therapy facilities using 100 and 125 MeV pencil beams delivered at minimum clinical currents. Polyethylene phantoms were irradiated at controlled positions and data were acquired during both in-spill and off-spill periods.
The first reconstructed 2D images demonstrate that PGI can directly identify the Bragg peak position through the maximum of the PGI distribution over a broad field of view, while PET provides a narrower and higher-resolution distribution associated with the induced beta+ activity. These results confirm the feasibility and complementarity of the hybrid PGI-PET approach and support its potential for accurate, clinically relevant proton range verification.
Keywords: Ion range verification, Positron Emission Tomography, Prompt Gamma Imaging, Proton therapy
12:49
M-LT-04-03
Intercrystal Compton Scattering Detection in Pixelated LYSO Detectors via Quantum Localization (#2993)
A. Hashemi1, X. Zhang1, H. Sabet1
1 Harvard Medical School/Massachusetts General Hospital, Radiology Department, Boston, Massachusetts, United States of America
Abstract
We introduce a novel quantum-inspired method for identifying intercrystal Compton scattering in pixelated scintillation detectors. The approach treats each SiPM readout as a spatial signal and converts it into a discrete eigenfunction representation using a Hamiltonian built from the measured intensity distribution. Event structure is then assessed through quantum localization, quantified by the participation ratio. Single-site events produce highly localized dominant modes, whereas Compton-scattered events produce multiple localized modes associated with distinct interaction sites. A dual criterion based on quantum localization and eigenvalue proximity is used to classify multi-site events without calibration-intensive response modeling or supervised training. The method was evaluated with Geant4 optical photon simulations and measurements from LYSO:Ce detector arrays with thicknesses from 2 to 25 mm. Experimental classification agreed closely with simulation, with differences below 1% for most thicknesses and below 5% in all cases. These results indicate that the proposed representation captures the topology of gamma-ray interactions directly from detector signals.
AcknowledgmentThis work was supported in part by NIH grant R01EB034785.
References [1] M. S. Lee, H. S. Shim, and J. S. Lee, “Strategies for mitigating inter-crystal scattering effects in positron emission tomography: a comprehensive review,” Biomedical Engineering Letters, vol. 14, no. 6, pp. 1243–1258, Nov. 2024, doi: 10.1007/s13534-024-00427-7. [2] S. Lee, K. Y. Kim, M. S. Lee, and J. S. Lee, “Recovery of inter-detector and inter-crystal scattering in brain PET based on LSO and GAGG crystals,” Phys. Med. Biol., vol. 65, no. 19, p. 195005, Oct. 2020, doi: 10.1088/1361-6560/ab9f5c. [3] M. N. Ullah and C. S. Levin, “Application of Artificial Intelligence in PET Instrumentation,” PET Clinics, vol. 17, no. 1, pp. 175–182, Jan. 2022, doi: 10.1016/j.cpet.2021.09.011. [4] A. Hashemi, S. Dutta, B. Georgeot, D. Kouamé, and H. Sabet, “A novel perspective on denoising using quantum localization with application to medical imaging,” AIP Advances, vol. 15, no. 8, p. 085012, Aug. 2025, doi: 10.1063/5.0267924. [5] A. Hashemi, S. Dutta, B. Georgeot, D. KouamÉ, and H. Sabet, “Quantum-Inspired Denoising via Adaptive Planck Constant and Image Patching,” in 2024 IEEE Nuclear Science Symposium (NSS), Medical Imaging Conference (MIC) and Room Temperature Semiconductor Detector Conference (RTSD), Oct. 2024, pp. 1–1. doi: 10.1109/NSS/MIC/RTSD57108.2024.10657709. [6] A. Hashemi, H. Babaei, and S. Lee, “Effects of medium range order on propagon thermal conductivity in amorphous silicon,” Journal of Applied Physics, vol. 127, no. 4, p. 045109, Jan. 2020, doi: 10.1063/1.5124821.
PETRARCA: a Positron Emission Tomography Real-Time Analog Re-Configurable ANN Detector (#2827)
M. Pandocchi1, 2, M. Amadori1, 2, M. Ronchi1, 2, G. Borghi1, 2, M. Carminati1, 2, C. Fiorini1, 2
1 Politecnico di Milano, Dipartimento di Elettronica Informazione e Bioingegneria, Milano, Italy 2 Istituto Nazionale di Fisica Nucleare, Sezione di Milano, Milano, Italy
Abstract
Positron emission tomography systems are becoming increasingly complex due to the growing number of detector channels and the large amount of data generated, especially in total-body imaging configurations. In this work, we present PETRARCA, a positron emission tomography detector system integrating an analog neural network ASIC (ANNA) for real-time edge computing of gamma-ray interaction coordinates within a monolithic scintillation crystal. The system consists of a 32 mm × 32 mm × 10 mm monolithic LYSO crystal coupled to an 8 × 8 SiPM matrix read out by dedicated front-end electronics. The detector architecture includes both a conventional digital acquisition path and a parallel analog inference path based on the ANNA ASIC, enabling simultaneous acquisition of sensor data and hardware neural-network predictions. A first evaluation of the system has been carried out using simulated data and the real ASIC response to emulate a reduced-scale configuration using a 4 × 4 SiPM array coupled to a 26 mm × 26 mm × 10 mm monolithic crystal. The performances of the ASIC in predicting the interaction coordinates were tested, and proved to have a mean absolute error (MAE) of around 1 mm on both the x and y axes. The preliminary results demonstrate the feasibility of analog neural-network edge computing for spatial localization in PET detectors and support further developments toward fully integrated real-time detector systems.
References [1] Nanni et al., “Total body positron emission tomography/computed tomography: Current status in oncology,” Semin. Nucl. Med., vol. 55, no. 1, pp. 31–40, 2025 [2] S. Di Giacomo et al., “Implementing an Integrated Neural Network for Real-Time Position Reconstruction in Emission Tomography With Monolithic Scintillators,” IEEE Trans. Radiat. Plasma Med. Sci., vol. 8, no. 5, pp. 501-510, May 2024. [3] A. Gonzalez-Montoro et al., “Evolution of PET detectors and event positioning algorithms using monolithic scintillation crystals,” IEEE Trans. Radiat. Plasma Med. Sci., vol. 5, pp. 282–305, 2021. [4] I. D’Adda et al., “SITH: An SiPM Readout ASIC for Prompt Gamma-Ray Detection in Hadrontherapy Applications,” IEEE Trans. Nucl. Sci., vol. 71, no. 9, pp. 2140–2150, 2024.
MIMOSA: Medical IMaging MOnte Carlo Simulation Algorithms for fast proton therapy range monitoring (#2751)
D. D. Garvey1, G. Llosá1, F. Hueso González1
1 IFIC, CSIC-UV, Valencia, Spain
Abstract
Monte Carlo simulations play a vital role in many aspects of proton therapy treatment, including proton depth of penetration monitoring. A key limiting factor of full simulation engines is computation time: simulations can take several days, far longer than the time between treatment fractions. This project aims to develop a Monte Carlo simulation software, MIMOSA, for prompt gamma-ray based proton range verification, that is fast enough to be deployed before the next treatment fraction. Clinically acceptable gamma pass rates above 99% for 2%/2 mm and 97% for 1%/1 mm with respect to TOPAS were achieved on both homogenous and heterogenous phantoms. To benchmark computational speed, state-of-the-art GPU codes MOQUI and FRED were tested on the same computer. Comparatively, MIMOSA achieved a notable speed increase, able to simulate 1e9 primary protons with a 200 MeV energy in approximately 3 minutes. Along with maintaining accuracy and increasing computational speed, the project uses the hardware agnostic SYCL standard, and will be available with an open-source license and extensive documentation. Ongoing work is devoted to simulating realistic radiotherapy treatment plans, and including prompt gamma-ray transport and detector response.
AcknowledgmentThis work has been funded by the Conselleria de Educación, Investigación, Cultura y Deporte (Generalitat Valenciana), Spain, under grant number CDEIGENT/2019/011, by CSIC's JAEPRE23-19 grant, and by the MIDAS project PID2022-143246OB-I00 (MICIU/AEI). IFIC is supported by the Severo Ochoa Center of Excellence grant CEX2023-001292-S funded by MCIU/AEI
References [1] F. Hueso-Gonzalez and T. Bortfeld, “Compact method for proton range verification based on coaxial prompt gamma-ray monitoring: A theoretical study,” IEEE Transactions on Radiation and Plasma Medical Sciences, vol. 4, no. 2, p. 170–183, Mar. 2020. [Online]. Available: http://dx.doi.org/10.1109/TRPMS.2019.2930362 [2] J. Perl, J. Shin, J. Schumann, B. Faddegon, and H. Paganetti, “TOPAS: An innovative proton Monte Carlo platform for research and clinical applications,” Medical Physics, vol. 39, no. 11, pp. 6818–6837, November 2012 [3] H. Lee, J. Shin, J. M. Verburg et al., “MOQUI: an open-source GPU-based Monte Carlo code for proton dose calculation with efficient data structure,” Physics in Medicine & Biology, vol. 67, no. 17, p. 175001, 2022, published August 30, 2022. [Online]. Available: https://doi.org/10.1088/1361-6560/ac8716 [4] M. D. Simoni, M. Fischetti, E. Gioscio, M. Marafini, R. Mirabelli, V. Patera, A. Sarti, A. Schiavi, A. Sciubba, and G. Traini, “FRED: A fast Monte Carlo code on GPU for quality control in particle therapy,” Journal of Physics: Conference Series, vol. 1548, no. 1, p. 012020, may 2020. [Online]. Available: https://doi.org/10.1088/1742-6596/1548/1/012020 [5] A. Alpay and V. Heuveline, “Adaptivity in AdaptiveCpp: Optimizing performance by leveraging runtime information during JIT-compilation,” in Proceedings of the 13th International Workshop on OpenCL and SYCL, ser. IWOCL ’25. New York, NY, USA: Association for Computing Machinery, 2025. [Online]. Available: https://doi.org/10.1145/3731125.3731127
Keywords: MIMOSA, open source, simulation, proton therapy, range verification
12:55
M-LT-04-06
Analytical modeling and inclusion of object scatter in non-TOF 3D PET for low-count data (#1275)
J. Roser1, H. P. Vo1, M. Rafecas1
1 Universität zu Lübeck, Institute of Medical Engineering, Lübeck, Schleswig-Holstein, Germany
Abstract
Compton scattering in Positron Emission Tomography (PET) is commonly seen as an important degrading factor for the image quality. In particular, object scattering is known to reduce image contrast and distort quantification. Conventional scatter correction techniques do not model scatter directly in the system matrix, despite its potential to better handle low-count data scenarios. In this work, we propose an analytical model for single Compton scattering events and subsequently derive expressions of the system matrix and sensitivity. We validate the obtained expressions with Monte Carlo simulations. Ongoing work includes studying the impact of such approach by using low-count simulated data, and a comparison of the proposed method with conventional scatter correction techniques.
AcknowledgmentThis work was supported by the European Union’s Horizon 2024 research and innovation programme under the Marie Skłodowska-Curie grant agreement no. 101207067, and partly by the German Research Foundation (DFG) under grant agreement no. 508064995.
References [1] Zaidi, H, Koral, KF 2004, ‘Scatter modelling and compensation in emission tomography’, Eur J Nucl Med Mol Imaging31, 761–782. DOI: 10.1007/s00259-004-1495-z [2] Watson, CC, et al. 1996, ‘A Single Scatter Simulation Technique for Scatter Correction in 3D PET’, In: Grangeat, P., Amans, JL. (eds) Three-Dimensional Image Reconstruction in Radiology and Nuclear Medicine. Computational Imaging and Vision, vol 4. Springer, Dordrecht. DOI: 10.1007/978-94-015-8749-5 [3] Tamal, M, et al. 2006, ‘Noise Properties of Four Strategies for Incorporation of Scatter and Attenuation Information in PET Reconstruction Using the EM-ML Algorithm’, IEEE Transactions on Nuclear Science, vol. 53, no. 5, pp. 2778-2786. DOI: 10.1109/TNS.2006.880973 [4] Markiewicz, PJ, et al. 2007, ‘High accuracy multiple scatter modelling for 3D whole body PET’, Phys. Med. Biol.52 829. DOI: 10.1088/0031-9155/52/3/021 [5] Schaar, M, Rafecas, M 2019, ‘Modelling of Scatter in the System Matrix for 3D PET Image Reconstruction: a Comparative Study’, 2019 IEEE Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC), Manchester, UK. DOI: 10.1109/NSS/MIC42101.2019.9059797 [6] Roser, J, et al. 2026, ‘Inclusion of Inter-crystal Scattering in PET: Analytical Models and Dedicated Reconstruction’, preprint. DOI: 10.48550/arXiv.2601.05717
Keywords: PET, object scatter, analytical model, sensitivity, system matrix
12:57
M-LT-04-07
Quantitative Impact of Inter-Crystal Scatter on Image Quality and Sensitivity across LabPET-II Scanner Architectures: A Comparative GATE Simulation Study (#2983)
A. Bernier1, 2, M. Gaudreault5, J.-F. Beaudoin3, R. Lecomte4, 5, J.-B. Michaud1, 2
1 University of Sherbrooke, Department of Electrical and Computer Engineering, Sherbrooke, Québec, Canada 2 University of Sherbrooke, Interdisciplinary Institute for Technological Innovation, Sherbrooke, Québec, Canada 3 CRCHUS, Sherbrooke Molecular Imaging Center, Sherbrooke, Sherbrooke, Québec, Canada 4 Imaging Research & Technology, Sherbrooke, Québec, Canada 5 University of Sherbrooke, Department of Medical Imaging and Radiation Sciences, Sherbrooke, Québec, Canada
Abstract
Inter-crystal scatter (ICS) is a primary limiting factor for spatial resolution and sensitivity in ultra-high resolution (UHR) PET imaging. This study provides a multiparametric quantification of ICS distributions across three successive LabPET-II scanner generations: Mouse, UHR, and SAVANT. Using GATE Monte Carlo simulations, we evaluate the complex tradeoff between substantial sensitivity gains and increased scatter contamination. Results demonstrate that while the SAVANT architecture provides a 39.9% increase in coincidence yield over the UHR, ICS events constitute 54.21% of total counts. These events are characterized through stable energy deposition profiles (approx. 0.326 MeV), multi-rank angular distributions, and a refined Line of Response (LOR) midpoint error metric.
A notable paradox is observed: the aggregate positioning error is lower for the SAVANT (11.01 mm) than for the UHR (12.22 mm), suggesting that the SAVANT's optimized geometric design constrains LOR deviations despite a higher scatter frequency. Furthermore, rank-based angular analysis confirms the invariance of primary physical signatures, with the first scattering angle ($\theta_0$) remaining remarkably consistent across all architectures (91.9° to 94.4°). This stability across the LabPET-II lineage establishes a robust physical framework for a universal deep learning-based positioning algorithm. By transforming scatter into a valuable signal rather than treating it as noise, this approach leverages the exceptional sensitivity of next-generation scanners to surpass current resolution limits through intelligent software processing.
AcknowledgmentThis work was supported in part by the Arbour foundation, the Faculty of Engineering and the Dept of electrical and computer engineering.
References [1] E. Gaudin et al. ”Performance Simulation of an Ultra-High Resolution Brain PET Scanner Using 1.2-mm Pixel Detectors” IEEE Trans Radiat Plasma Med Sci, vol. 3, no.3, pp. 334-342, 2018 [2] R. Lecomte, ”First Results from the SAVANT Ultra-High-Resolution Phoswich-Based DOI Brain PET Scanner,” Oral presented at FTMI-TBPET-PSMR, Valencia, Spain, May 2026 [3] S. Jan et al., ”GATE V6: a major enhancement of the GATE simulation platform,” Phys. Med. Biol., vol. 56, no. 4, pp. 881-901, 2011
Keywords: Inter-Crystal Scatter (ICS), Monte Carlo Simulations (GATE), LabPET-II Architectures, Positioning Accuracy, Deep Learning Priors
12:59
M-LT-04-08
Validated Optical Simulation for High-Energy Gamma Response in a 3-Layer LYSO DOI Detector (#1668)
S. Jiang1, G. Lovatti1, F. Evangelista1, P. Thirolf1, K. Parodi1, M. Nitta1
1 Ludwig-Maximilians-Universität München, München, Bavaria, Germany
Abstract
We have developed a 3-layer staggered LYSO de tector with DOI capability within the project SIRMIO (Small animal proton irradiator for research in molecular image-guided radiation-oncology) for proton range verification via PET imag ing. To evaluate the feasibility of detecting prompt gamma rays for quasi-instantaneous monitoring of proton beams, we propose a workflow that includes the validation of optical simulation settings and the implementation of the saturation effect of the SiPM photonsensor in the Geant4 simulation. Measurement data with 152Eu, 22Na and 137Cs radioactive sources are utilized for modeling the saturation effect of SiPM, and also for validating optical boundary settings in Geant4. The measured spectra of 22Na and 137Cs point sources are well reproduced with the proposed simulation workflow. The responses to prompt gamma rays are then simu lated. According to the floodmaps and profiles, LYSO pixel can be identified at 2.2, 4.4 and 6.2 MeV, but the contrast decreases strongly when energy reaches 6.2 MeV. The peak-to-valley ratios drop by up to 53% at 4.4 MeV and 62% at 6.2 MeV (relative to 2.2 MeV), primarily due to the energy deposition occurring more frequently in multiple LYSO pixels. These predictions suggest the detector’s potential for detecting prompt gamma rays, while accurately recovering or rejecting inter-crystal scatter events is essential to maintain detector performance at higher gamma energy.
References [1] K. Parodi et al., Acta Oncol., vol. 58, no. 10, p. 1470, 2019. [2] T. M. Fitzpatrick, Ph.D. dissertation, lmu, 2022. [3] J. Allison et al., Nucl. Instrum. Meth. A, vol. 835, p. 186, 2016. [4] K. Kotera et al., arXiv:1510.01102, 2015. [5] M. Janecek et al., IEEE Trans. Nucl. Sci., vol. 57, no. 3, p. 964, 2010.
Identification of ICS Pixels in a high-resolution 3-Layer DOI-PET Detector Using a CNN (#2619)
S. Jiang1, G. Lovatti1, F. Evangelist1, P. Thirolf1, K. Parodi1, M. Nitta1
1 Ludwig-Maximilians-Universität München, München, Bavaria, Germany
Abstract
We have developed a 3-layer staggered LYSO DOI detector for the SIRMIO (Small animal proton irradiator for research in molecular image-guided radiation-oncology) project, with a crystal pitch of 1.0 mm. Due to the small crystal size, inter-crystal scatter (ICS) events degrade spatial resolution, while discarding them causes significant sensitivity loss. In our detector, ICS events account for approximately 50% of all interactions at 511 keV and result in a median lateral positioning error of approximately 2 mm. To solve this problem, we propose a dual-head convolutional neural network (CNN) for separating the 8×8 MPPC total response of two-pixel ICS events into two individual response matrices, from which the pixel positions and energy fractions can be obtained—a precondition for recovering the ICS events. The CNN correctly identifies both scattering pixels in 69.3% of test events, and in 26.4% of cases one pixel is correctly identified. Among the events with one pixel mismatched, the lateral error of the misidentified pixel falls within 1.0 mm in 91.0% of cases. Meanwhile, the median energy fractions prediction error is 0.016 per pixel. The results demonstrate that CNN-based MPPC response decomposition can serve as the enabling foundation for complete ICS recovery in 3-layer staggered DOI detectors, addressing a limitation explicitly acknowledged in recent physics-based ICS studies.
References [1] F. Evangelista et al., in 2024 IEEE NSS MIC RTSD, 2024. [2] K. Parodi et al., Acta Oncol., vol. 58, no. 10, p. 1470, 2019. [3] M. S. Lee et al., Biomedical Engineering Letters, vol. 14, no. 6, 2024. [4] Q. Liu et al., Physics in Medicine and Biology, 2026. [5] S. Jiang et al., submitted to IEEE NSS MIC RTSD 2026 (#1668).
Study on the axial extension of the small-fish PET scanner MERMAID (#2065)
M. Kolodziej1, J. Roser1, S. Seeger1, 2, H. P. Vo1, R. Kantorek1, 2, M. Rafecas1
1 University of Luebeck, Institute of Medical Engineering, Luebeck, Schleswig-Holstein, Germany 2 University of Luebeck, Isotope Laboratory of the Natural Science Section, Luebeck, Schleswig-Holstein, Germany
Abstract
MERMAID is the first PET scanner prototype dedicated to study small aquatic animals. Particularly, it aims to support the use of adult zebrafish as a model of human diseases. The current prototype, which consists of four detection modules composed of LYSO:Ce crystals, has demonstrated the capability of providing images with submillimeter resolution. An extension of MERMAID by another four modules is planned, aimed to increase the system sensitivity and allow for shorter scan times, making it more suitable for in-vivo imaging. In the presented work, various configurations for the extended MERMAID system are characterized by means of simulations and tailored reconstruction framework; modifications of imaging protocol for the system are investigated.
AcknowledgmentThe project is partially supported by the German Research Foundation (DFG) under grant agreement no. 496099829 and the DFG Cluster of Excellence PMI under grant agreement no. 390884018.
References [1] S. Seeger et al., 2023 IEEE NSS MIC RTSD, 2023. doi: 10.1109/NSSMICRTSD49126.2023.10338697. [2] J. Roser et al., IEEE TRPMS, 2026. doi: 10.1109/TRPMS.2026.3691192.