Background: Grid therapy has in the past normally been performed with single field photon-beam grids. In this work, we evaluated a method to deliver grid therapy based on interlacing and crossfiring grids of mm-wide proton beamlets over a target volume, by Monte Carlo simulations.
Material And Methods: Dose profiles for single mm-wide proton beamlets (1, 2 and 3 mm FWHM) in water were simulated with the Monte Carlo code TOPAS. Thereafter, grids of proton beamlets were directed toward a cubic target volume, located at the center of a water tank. The aim was to deliver a nearly homogeneous dose to the target, while creating high dose heterogeneity in the normal tissue, i.e., high gradients between valley and peak doses in the grids, down to the close vicinity of the target.
Results: The relative increase of the beam width with depth was largest for the smallest beams (+6.9 mm for 1 mm wide and 150 MeV proton beamlets). Satisfying dose coverage of the cubic target volume (σ < ±5%) was obtained with the interlaced-crossfiring setup, while keeping the grid pattern of the dose distribution down to the target (valley-to-peak dose ratio <0.5 less than 1 cm before the target). Center-to-center distances around 7-8 mm between the beams were found to give the best compromise between target dose homogeneity and low peak doses outside of the target.
Conclusions: A nearly homogeneous dose distribution can be obtained in a target volume by crossfiring grids of mm-wide proton-beamlets, while maintaining the grid pattern of the dose distribution at large depths in the normal tissue, close to the target volume. We expect that the use of this method will increase the tumor control probability and improve the normal tissue sparing in grid therapy.
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http://dx.doi.org/10.1080/0284186X.2017.1350287 | DOI Listing |
Cancers (Basel)
November 2024
Radiotherapy and Radiation Dosimetry, National Physical Laboratory, Teddington TW11 0LW, UK.
J Appl Clin Med Phys
January 2025
Department of Radiation Oncology, University of Iowa, Iowa City, Iowa, USA.
Purpose: To computationally characterize the LET distribution during dynamic collimation in PBS and quantify its impact on the resultant dose distribution.
Methods: Monte Carlo simulations using Geant4 were used to model the production of low-energy proton scatter produced in the collimating components of a novel PBS collimator. Custom spectral tallies were created to quantify the energy, track- and dose-averaged LET resulting from individual beamlet and composite fields simulated from a model of the IBA dedicated nozzle system.
Radiother Oncol
January 2025
Physics Division, Department of Radiation Oncology, Massachusetts General Hospital & Harvard Medical School, Boston, MA, USA. Electronic address:
Background And Purpose: Proton arc therapy and FLASH radiotherapy (FLASH-RT) each offer unique advantages in proton therapy. However, clinical translation of FLASH-RT faces challenges in defining and delivering high dose rates. We propose the use of proton FLASH-arc therapy (PFAT) to leverage the benefits of arc while addressing FLASH delivery concerns by spatially fractionating dose delivery to healthy tissue.
View Article and Find Full Text PDFPhys Med Biol
August 2024
Paul Scherrer Institute, Villigen, Switzerland.
To experimentally validate two online adaptive proton therapy (APT) workflows using Gafchromic EBT3 films and optically stimulated luminescent dosimeters (OSLDs) in an anthropomorphic head-and-neck phantom.A three-field proton plan was optimized on the planning CT of the head-and-neck phantom with 2.0 Gy(RBE) per fraction prescribed to the clinical target volume.
View Article and Find Full Text PDFMed Phys
October 2024
Department of Radiation Oncology, University of Kansas Medical Center, Kansas City, USA.
Background: Proton spatially fractionated RT (SFRT) can potentially synergize the unique advantages of using proton Bragg peak and SFRT peak-valley dose ratio (PVDR) to reduce the radiation-induced damage for normal tissues. Uniform-target-dose (UTD) proton GRID is a proton SFRT modality that can be clinically desirable and conveniently adopted since its UTD resembles target dose distribution in conventional proton RT (CONV). However, UTD proton GRID is not used clinically, which is likely due to the lack of an effective treatment planning method.
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