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Three-dimensional computational evaluation of water-to-air mass stopping power ratio for therapeutic helium-, carbon-, oxygen-, and neon-ion beams and its application to patient-specific quality assurance

In brief

Ion-beam calculations find suitable stopping ratios of 1.128 to 1.129

In treatment-plan simulations, the average water-to-air stopping power ratio within targets was 1.128 for carbon and oxygen ions and 1.129 for helium and neon ions, rather than the standard 1.126. Ratios varied across the target, with shallow neon plans sometimes exceeding the standard uncertainty range in a small distal region; patient-specific calculations could refine quality assurance, but clinical impact remains untested.

Journal
Physics in medicine and biology (Q1)
Published
30 October 2026
Study design
Unclassified
Evidence level
Level 5, Expert Opinion (CEBM 5)
Authors
Taku Inaniwa, Makoto Sakama, Nobuyuki Kanematsu
PMID
42962366
DOI
10.1088/1361-6560/aebc07

Why clinicians should know about it

  • Picked for Medical Physics (paper of the day, 31 October 2026): Ion-beam stopping-power modeling supports patient-specific QA

Abstract

Current dosimetry protocols recommend a constant water-to-air mass stopping power ratio, sw,air, of 1.126 with an uncertainty of ±1.5% for light ions, irrespective of ion species and energy. This study aims to develop a computational framework to calculate three-dimensional sw,air distributions of helium-, carbon-, oxygen-, and neon-ion beams for patient specific quality assurance (PSQA), and to systematically investigate spatial variations in sw,air under clinically relevant conditions. 
Approach. A computational framework was developed to calculate three-dimensional sw,air distributions based on the Bragg-Gray approximation, together with three-dimensional dose distributions for treatment planning. The framework was validated against published datasets for a mono-energetic carbon-ion beam. Treatment plans were generated using helium-, carbon-, oxygen-, and neon-ion beams for rectangular targets with varying spread-out Bragg peak (SOBP) widths and depths, as well as for bone and soft tissue, head and neck, and ocular cases. The corresponding sw,air distributions were calculated in a water phantom and compared with the recommended value of 1.126. 
Main Results. The mean sw,air within the target increased for shallower targets with narrower SOBP widths. For all ion species, sw,air increased toward the distal end of the SOBP, with larger variations observed for heavier ion species. In neon-ion irradiations for shallow targets, sw,air occasionally exceeded the ±1.5% uncertainty range in a limited region near the distal end of the SOBP. In all other cases, sw,air remained within the uncertainty range. Similar trends were observed in clinical cases. Based on these results, when considering the mean sw,air within the target, the suitable fixed values were 1.128 for carbon and oxygen ions and 1.129 for helium and neon ions. 
Significance. The proposed computational framework enables three-dimensional, plan-specific evaluation of sw,air and provides a practical approach for improving the dosimetric accuracy in charged-particle therapy with helium, carbon, oxygen, and neon ions, especially for PSQA.&#xD.

Abstract as published, via PubMed.

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For healthcare professionals. The summary is generated by AI from the published abstract, and the evidence level is assigned automatically from the study design on the Oxford CEBM hierarchy. Neither is medical advice. Read the full paper before changing practice.