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Updated: Jun 13, 2025

Registered Bioimaging of Nanomaterials for Diagnostic and Therapeutic Monitoring
Published on: December 9, 2010
Real-time radiation beam imaging on an MR linear accelerator using quantitative T1 mapping
Brandon T T Tran1,2, Liam S P Lawrence1,2, Shawn Binda3
1Physical Sciences Platform, Sunnybrook Research Institute, Toronto, ON, Canada.
Background:
Direct three-dimensional imaging of radiation beams could enable more accurate radiation dosimetry. It has been previously reported that changes in T1-weighted magnetic resonance imaging (MRI) intensity could be observed during radiation due to radiochemical oxygen depletion. Quantitative T1 mapping could increase sensitivity for dosimetry applications.
Purpose:
We use an MRI linear accelerator (MR-Linac) to visualize radiation delivery through the real-time effects of dose on the spin-lattice magnetic relaxation time (T1) of water. We quantify the relationships between dose, spin-lattice relaxation rates (R1) and dissolved oxygen concentration to further investigate the mechanisms of T1 change.
Methods:
An ultrapure water phantom and a 1% agarose gel phantom were irradiated and imaged on a 1.5 T Elekta Unity MR-Linac. Radiation plans were created using the Monaco treatment planning system. Images were acquired before, during and after radiation. A dual-echo Look-Locker inversion recovery pulse sequence was used for simultaneous dynamic T1/B0 mapping. The change in R1 with respect to dose (∆R1/∆Dose) and the radiochemical oxygen depletion (ROD = ∆O2/∆Dose) were measured. The relaxivity of oxygen (r1,O2 = ∆R1/∆O2) in water was also measured in a separate experiment with samples of various dissolved oxygen concentrations. The minimum measurable dose over a 20-min period was estimated using a single-tailed 99th quantile Student's t-distribution.
Results:
Changes to R1 were found to be spatiotemporally correlated to the predicted delivered radiation dose and persisted for at least 1 h after radiation. A complex dose plan could be imaged in the 1% agarose gel phantom, as the gel limits diffusion and convective mixing. In water, the ∆R1/∆Dose was found to be -1.0 × 10-4 s-1/Gy, the r1,O2 was found to be 5.4 × 10-3 s-1/(mg/L), and the ROD was found to be -0.010 (mg/L)/Gy. Both r1,O2 and ROD agree with published values. However, combining these two values yields a predicted ∆R1/∆Dose of -5.4 × 10-5 s-1/Gy, indicating that radiochemical oxygen depletion alone under-predicts the MRI effect. The detection limit of R1 was 1.1 × 10-3 s-1 which corresponded to a single-voxel minimum detectable dose of 11.1 Gy for this specific sequence.
Conclusion:
Quantitative T1 mapping was used to image radiation dose patterns in real-time in water and agarose gel. Radiochemical oxygen depletion only partially explains the T1 changes measured. Agarose gel could be used as a simple system for three-dimensional patient-specific quality assurance. Future applications may include in vivo dosimetry for FLASH radiotherapy, though improvements in acquisition methods and hardware are likely needed.
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