ESTRO 2023 - Abstract Book

S1763

Digital Posters

ESTRO 2023

Conclusion PDASC demonstrated its computation efficiency in the high-sparsity solutions, in which SPArc treatment delivery efficiency is a high priority in the proton routine clinical practice.

PO-1990 Monitoring and Quality Assurance of scanned proton pencil beams using a CMOS detector

S. Flynn 1,2 , C. Baker 3,4 , M. Homer 1 , V. Rompokos 3,4 , R. Thomas 1,5 , A. Toltz 3,4 , T. Price 2,1

1 National Physical Laboratory, Medical Radiation Science, Teddington, United Kingdom; 2 University of Birmingham, Particle Physics, Birmingham, United Kingdom; 3 University College London Hospitals NHS Foundation Trust, Department of Radiotherapy Physics, London, United Kingdom; 4 University College London, Department of Medical Physics and Biomedical Engineering, London, United Kingdom; 5 University of Surrey, Faculty of Engineering and Physical Sciences, Guildford, United Kingdom Purpose or Objective The effectiveness of Pencil Beam Scanning (PBS) proton beam therapy is highly dependent upon delivering a uniform dose distribution to a target volume. This requires confidence in both the positional accuracy and the shape of the pencil beam, as an error of either could compromise dose coverage to the target. Current on-line beam monitoring for PBS uses multiple one dimensional detectors for measuring and confirming proton beam positions and profiles upstream of the target volume, but this lacks the ability to provide true two dimensional validation of the pencil beam shape and position. Complementary Metal–Oxide–Semiconductor (CMOS) detector with 50 µm pixel pitch was evaluated for PBS proton delivery in a Varian ProBeam® gantry. The CMOS detector was placed as close to the beam nozzle as possible. To prevent pixel saturation, the pixel integration time was reduced to 1.8 ms/frame by restricting the region of interest. Results The CMOS detector was first exposed to a series of monoenergetic QA beam deliveries with varying energy, spot separation, and Monitor Units (MU) per spot. The CMOS detector was able to measure clinical beams up to approximately 180 MeV without saturation. In 70 and 150 MeV beams, the CMOS detector was able to measure in two dimensions without saturation, allowing spot separation to be tested and verified (Figure 1). Current dead time between consecutive frames of 14 ms results in approximately 30% of spot positions missed at 50 MU/spot, increasing to 80% of spot positions missed at 10 MU/spot. To identify treatment delivery error monitoring potential, the CMOS detector to identify treatment delivery errors, a QA plan (150 MeV, 50 MU/spot, 2.5 mm spot separation, 10 × 10 cm ² field) was manually edited by the clinical staff to distort one spot position by 1.0 mm in one axis. Information about the location and direction of this spot was intentionally withheld from the team conducting the CMOS analysis. The misaligned beam can be identified as the antepenultimate spot in the x -axis. Due to the position of the CMOS detector in the nozzle, the measured distortion was 0.77±0.01 mm. Materials and Methods The vM2428 ”LASSENA”, a large-format