Abstract

Up to now, carbon ions have shown the most favorable physical and radiobiological properties for radiation therapy of, for example, deep-seated radioresistant tumors. However, when carbon ions penetrate matter, they undergo inelastic nuclear reactions that give rise to secondary fragments contributing to the dose in the healthy tissue. This can cause damage to radiosensitive organs at risk when they are located in the vicinity of the tumor. Therefore, predictions of the yields and angular distributions of the secondary fragments are needed to be able to estimate the resulting biological effects in both the tumor region and the healthy tissues. This study presents the accuracy of simulations of therapeutic carbon ion beams with water, with the 3D MC (Monte Carlo) general purpose particle and ion transport code PHITS. Simulations with PHITS of depth-dose distributions, beam attenuation, fragment yields, and fragment angular distributions from interactions of therapeutic carbon ion beams with water are compared to published measurements performed at Gesellschaft für Schwerionen Forschung (GSI). The results presented in this study demonstrate that PHITS simulations of therapeutic carbon ion beams in water show overall a good agreement with measurements performed at GSI; for example, for light ions like H and He, simulations agree within about 10%. However, there is still a need to further improve the calculations of fragment yields, especially for underproduction of Li of up to 50%, by improving the nucleus-nucleus cross-section models. The simulated data are clinically acceptable but there is still a need to further improve the models in the transport code PHITS. More reliable experimental data are therefore needed.

Highlights

  • Carbon ion therapy has shown to be very promising for treating a wide variety of tumors, especially deep-seated and radioresistant ones, and by the end of 2016 nearly 20 000 patients had been treated with carbon ions worldwide [1]

  • Comparisons of Depth-Dose Distributions and Beam Fluence Attenuation In Figure 2, the Bragg curves of 400-MeV/u 12C ions in water are displayed as predicted by Particle and Heavy Ion Transport code System (PHITS) together with experimental data [6, 7]

  • PHITS simulations of depth-dose distributions, fragment yields, and angular distributions from the interactions of therapeutic (400 MeV/u) carbon ion beams with water are compared to measurements performed at Gesellschaft fur Schwerionen Forschung (GSI) by Haettner et al [6] and Haettner [7]

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Summary

Introduction

Carbon ion therapy has shown to be very promising for treating a wide variety of tumors, especially deep-seated and radioresistant ones, and by the end of 2016 nearly 20 000 patients had been treated with carbon ions worldwide [1] This success is due to a number of advantages when using heavy ions for radiation therapy compared to photon or proton radiation therapy. The specific ionization increases with decreasing particle velocity, giving rise to a sharp maximum (Bragg peak) in ionization near the end of range. This property makes it beneficial to use charged particles, for example, protons or heavier ions, to treat deep-seated tumors. The sharpness of the lateral dose fall-off, often called apparent penumbra, is of clinical importance because the radiation exposure to normal tissues adjacent to the target volume often limits the therapy dose, especially for a tumor close to critical organs

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