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30 June 2024 to 4 July 2024
FMDUL
Europe/Lisbon timezone

Experimental LET characterization with Minipix Timepix3 for quality assurance in proton therapy

3 Jul 2024, 14:41
1m
Main Auditorium (FMDUL)

Main Auditorium

FMDUL

Main Auditorium of the Faculty of Dental Medicine at the University of Lisbon (Faculdade de Medicina Dentária da Universidade de Lisboa)

Speaker

Ms Paulina Stasica (The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences, Cyclotron Centre Bronowice, Krakow, Poland)

Description

Purpose
As proton therapy is increasingly more popular around the world, there is a push towards advancement in quality assurance and control procedures that would include radiation quality besides standard physical dose verification. The spectrum of linear energy transfer (LET) of protons can provide comprehensive information on radiation quality in a given voxel. The spectral information and tracking response provided by Timepix detector technology allow for experimental high-resolution LET characterization of single protons [1] in complex and mixed radiation fields. In this work, we applied a Timepix3 detector to characterize proton LET spectra in mixed radiation fields produced in a water-equivalent phantom by clinical proton beams.

Methods
The spectral-sensitive particle tracking technique and the artificial neural network-based particle identification model allow for the experimental characterization of LET for single protons in mixed radiation fields [2, 3]. Here, we used a Minipix Timepix3 detector in Flex configuration (figure 1a) with a 300 μm silicon sensor calibrated with customized DAC settings and operated in data-driven mode. We performed measurements for a homogenous layer irradiated with a 164.6 MeV proton beam behind a solid RW3 phantom (figure 1a) with the detector sensor positioned in the middle of the layer at 45° to the beam direction (figure 1b). We compared deposited energy and LET spectra obtained based on measurements and Monte Carlo (MC) simulations performed with fast, GPU-accelerated FRED MC code [4] and implemented beam model [5].

Results
An accuracy of over 95% was obtained for proton recognition, and a broad spectrum of LET values was observed from a fraction of keV/μm to about ten keV/μm in mixed radiation fields produced by proton beam in water [1, 2]. A good agreement was obtained between measurement and simulation results for both deposited energy and proton LET spectra, as presented in figure 1 c and d, respectively.

enter image description here
Figure 1. Measurement setup at CCB IFJ PAN consisting of a solid RW3 phantom with a Minipix Timepix3 Flex detector (a). Calculated (MC simulation) relative dose distribution for a homogenous layer irradiated with a 164.6 MeV proton beam with marked sensor position (b). Comparison of the proton energy deposition (c) and LET spectra (d) for measurements (blue) and simulations (orange).

Conclusions
Experimental characterization of LET spectra within the clinical setting of proton therapy is needed for quality assurance and control of treatment plans that are optimized with both dose and LET. The Timepix detector provides a unique possibility of tracking individual particles in mixed radiation fields and characterizing proton LET spectra at a given point. The presented approach provides experimental solutions for LET characterization to support advancement in proton therapy treatment planning.

Acknowledgments
Work in CCB IFJ PAN was supported by the National Center for Research and Development (NCBiR) within grant No. LIDER/43/0222/L-12/20/NCBR/2021. Work in Advacam was performed in the frame of Contract No. 4000130480/20/NL/GLC/hh from the European Space Agency.

References

  1. C. Granja et al. (2021), NIM-A, vol. 988, pp. 164901
  2. P. Stasica et al. (2023), Phys. Med. Biol., vol. 68, no. 10, pp. 104001
  3. A. Rucinski et al. (2023), Int. J. Part. Ther., vol. 10 (2), pp. 118-396
  4. A. Schiavi et al. (2017), Phys. Med. Biol. vol. 62, no 18, pp. 7482–7504
  5. J. Gajewski et al. (2021), Int. J. Part. Ther., vol. 10 (2), pp. 118-396

Primary authors

Ms Paulina Stasica (The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences, Cyclotron Centre Bronowice, Krakow, Poland) Dr Antoni Rucinski (The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences, Cyclotron Centre Bronowice, Krakow, Poland) Prof. Damian Borys (The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences, Cyclotron Centre Bronowice, Krakow, Poland, Silesian University of Technology, Department of Systems Biology and Engineering, Gliwice, Poland) Prof. Carlos Granja (ADVACAM, Research and Development Department, Prague, Czech Republic) Ms Angelica De Gregorio (Dipartimento di Scienze di Base e Applicate per Ingegneria, Sapienza Universita di Roma, Roma, Italy) Prof. Renata Kopeć (The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences, Cyclotron Centre Bronowice, Krakow, Poland) Mr Dawid Krzempek (The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences, Cyclotron Centre Bronowice, Krakow, Poland) Mr Lukas Marek (ADVACAM, Research and Development Department, Prague, Czech Republic, Charles University, Faculty of Mathematics and Physics, Prague, Czech Republic) Dr Hanh Nguyen (Baylor University, Electrical and Computer Engineering Department, Waco, United States of America) Dr Cristina Oancea (ADVACAM, Research and Development Department, Prague, Czech Republic) Mr Łukasz Raczyński (The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences, Cyclotron Centre Bronowice, Krakow, Poland) Dr Marzena Rydygier (The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences, Cyclotron Centre Bronowice, Krakow, Poland) Prof. Angelo Schiavi (Dipartimento di Scienze di Base e Applicate per Ingegneria, Sapienza Universita di Roma, Roma, Italy) Prof. Keith Schubert (Baylor University, Electrical and Computer Engineering Department, Waco, United States of America) Prof. Reinhard Schulte (Loma Linda University, Loma Linda, CA, United States of America) Mr Maciej Sumera (The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences, Cyclotron Centre Bronowice, Krakow, Poland) Dr Jan Gajewski (The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences, Cyclotron Centre Bronowice, Krakow, Poland)

Presentation materials