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Updated: Sep 12, 2026

Tumor Hypoxia Assessment: In Vivo 3D Oxygen Imaging Through Electron Paramagnetic Resonance
Published on: February 14, 2025
A Mechanism-Guided Approach for Quantifying the Biological Effects of Tumor Hypoxia in Particle Therapy
Fada Guan1, Robert D Stewart2, David J Carlson3
1Department of Radiation Physics, The University of Texas MD Anderson Cancer Center, Houston, Texas.
Purpose:
To quantify how acute tumor hypoxia modifies the biological effectiveness of proton, helium, and carbon ions and to derive mechanistic hypoxia-compensation factors for representative spread-out Bragg peaks.
Methods And Materials:
The Monte Carlo Damage Simulation was used to generate DNA double-strand break yields as functions of radiation quality q = (Zeff/β)2 and oxygen level pO2 (0.0001%-100%). Monte Carlo Damage Simulation-derived double-strand break yields were integrated into Geant4 Monte Carlo simulations, and Repair-Misrepair-Fixation model calculations were used to derive linear-quadratic radiosensitivity parameters. We distinguish hypoxic RBE (RBEH), which compares the biological effects of particles at reduced pO2 with photons under normoxic conditions (137Cs γ-rays at pO2 = 100%), from isoeffective RBE (RBEiso), which compares particles and photons at the same pO2. Spread-out Bragg peak (10-15 cm depth) optimizations used either a uniform 2 Gy absorbed dose or a uniform RBEH-weighted dose (DRBE = 3.8 Gy) corresponding to 10% clonogenic survival in H460 cells; hypoxia reduction factors quantified the absorbed-dose compensation required to preserve this modeled endpoint.
Results:
At pO2 = 21%, at DRBE = 3.8 Gy, RBEH was 1.04-1.16 for protons, 1.23-1.67 for helium ions, and 1.84-3.55 for carbon ions. At pO2 = 0.001%, RBEH decreased to 0.39-0.41, 0.50-0.70, and 0.87-2.28, respectively. Because RBEH uses the fixed photon reference at pO2 = 100%, values below unity quantify the combined oxygen and radiation-quality penalty and do not indicate that particles are less effective than photons irradiating the same hypoxic tissue. At pO2 = 0.001%, RBEiso remained >1 (protons 1.13-1.19; helium 1.46-2.03; carbon 2.54-6.63). The corresponding hypoxia reduction factors were 2.73-2.89, 2.42-2.53, and 1.57-2.07.
Conclusions:
Within the H460 single-fraction clonogenic-survival framework examined here, high-LET carbon ions are less sensitive to severe hypoxia than helium ions or protons and require smaller model-derived hypoxia-compensation factors.
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