MBMateusz Bala

Mateusz Bala

*This is an algorithmically generated author record based on publicly available information.

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Previous Organizations / Institutes

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Mateusz Bala has a total of 43 co-authors. Here are the top co-authors by number of shared publications:


Latest Publications

  • Open Access

    A Monte Carlo positronium decay source model with multiple annihilation channels in GATE

    by Wojciech Krzemien, Mateusz Bala, Kamil Dulski, Wojciech Zdeb, Aurélien Coussat, Beatrix C Hiesmayr, Konrad Klimaszewski, Michał Obara, L Raczyński, Roman Y Shopa

    Objective . Positronium-based imaging, including positronium lifetime imaging (PLI) and multi-photon positron emission tomography (PET), requires realistic modelling of positronium (Ps) decay in matter. Existing Monte Carlo (MC) implementations in Geant4 Application for Tomographic Emission (GATE) are limited to simplified single- or two-channel descriptions, preventing accurate representation of the multi-component lifetime structure observed in biological and material systems. The objective of this work is to develop and validate a flexible MC Ps decay source model supporting multiple annihilation channels within the GATE framework. Approach . We introduce a modular Ps decay model implemented in GATE 9.4 and GATE 10, enabling the definition of an arbitrary number of decay channels characterised by lifetime, branching fraction, annihilation multiplicity ( 2 γ / 3 γ ), and optional prompt photon emission. The model is validated through analytical and numerical benchmarks, including lifetime distributions, branching fraction consistency, photon kinematics, and prompt photon emission. Its practical applicability is demonstrated using simulations of mixed annihilation scenarios and the NEMA IEC phantom with a large field-of-view PET system. Results . The proposed model accurately reproduces input lifetime distributions as weighted sums of exponential components and correctly samples decay channel fractions. Simulated two- and three-photon annihilation kinematics are consistent with theoretical expectations. Complex mixtures of decay channels, including varying 3 γ -to- 2 γ ratios and multi-component ortho-positronium (o-Ps) lifetimes, are correctly modelled, with observable signatures reflected in both temporal and energy distributions. Phantom simulations demonstrate the capability to generate realistic positronium-sensitive datasets. Significance . This work provides the first general-purpose, multi-channel positronium decay model integrated into GATE, enabling realistic simulations of positronium behaviour in complex media. The model supports the development and optimisation of positronium-based imaging techniques, including PLI and multi-photon PET, and applies to medical imaging, industrial tomography, and fundamental physics studies. Its public availability and compatibility with standard GATE workflows make it a valuable tool for the broader research community.

  • Open Access

    Probing arbitrary polarized photon pairs undergoing double Compton scatterings by a dedicated MC simulator validated with experimental data

    by Mateusz Bała, Wojciech Krzemień, Beatrix C. Hiesmayr, Jakub Baran, Kamil Dulski, Konrad Klimaszewski, Lech Raczyński, Roman Y. Shopa, Wojciech Wiślicki

    Quantum correlations in the polarization degree of freedom of the two-photon system have been extensively studied and form our current understanding of the quantum nature of our world. Most of the studies are concentrated on the low-energy (optical) photon pairs, for which efficient polarization measurement devices exist. However, for high-energetic (MeV) pairs of photons, e.g. produced in the decay of positronium atoms, no polarizers are available. Partial information about the polarization degree of freedom can be extracted by exploiting the measurements of photon pairs that undergo double Compton scattering. We present a Geant4-based Monte Carlo Vienna–Warsaw model capable of simulating any initial polarization state of bipartite photons. This puts us in a position to derive the behavior of the experimental observable, the angular difference $$\Delta \hat{\Phi }$$ Δ Φ ^ formed by the two scattering planes. We validate our Vienna–Warsaw simulator with the high-statistics experimental sample – based on a total of $$3 \times 10^5 $$ 3 × 10 5 event candidates – of two-photon pairs measured with the J-PET Big Barrel detector. We deduce the value of the squared visibility (interference contrast) encoding the polarization in the angle difference of the two scattering planes, $$\Delta \hat{\Phi }$$ Δ Φ ^ . The simulated spectra are in good agreement with the experimental correlation spectra and behave as predicted by theory.


  • Synchronization and Calibration of the 24-Modules J-PET Prototype With 300-mm Axial Field of View

    by P. Moskal, T. Bednarski, Sz. Niedzwiecki, M. Silarski, E. Czerwinski, T. Kozik, J. Chhokar, M. Bala, C. Curceanu, R. Del Grande, et al.

    Research conducted in the framework of the J-PET project aims to develop a cost-effective total-body positron emission tomography scanner. As a first step on the way to construct a full-scale J-PET tomograph from long strips of plastic scintillators, a 24-strip prototype was built and tested. The prototype consists of detection modules arranged axially forming a cylindrical diagnostic chamber with the inner diameter of 360 mm and the axial field-of-view of 300 mm. Promising perspectives for a low-cost construction of a total-body PET scanner are opened due to an axial arrangement of strips of plastic scintillators, wchich have a small light attenuation, superior timing properties, and the possibility of cost-effective increase of the axial field-of-view. The presented prototype comprises dedicated solely digital front-end electronic circuits and a triggerless data acquisition system which required development of new calibration methods including time, thresholds and gain synchronization. The system and elaborated calibration methods including first results of the 24-module J-PET prototype are presented and discussed. The achieved coincidence resolving time equals to CRT = 490 ± 9 ps. This value can be translated to the position reconstruction accuracy σ(Δ) = 18 mm which is fairly position-independent Keywords: positron emission tomography, plastic scintillators, J-PET.