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磁共振直线加速器中电离室角响应的实验测量及其相关磁场校正因子

Experimental measurement of ionization chamber angular response and associated magnetic field correction factors in MR-linac.

机构信息

Odette Cancer Centre, Sunnybrook Health Sciences Centre, Toronto, ON, M4N 3M5, Canada.

Department of Radiation Oncology, University of Toronto, Toronto, ON, M4N 3M5, Canada.

出版信息

Med Phys. 2020 Apr;47(4):1940-1948. doi: 10.1002/mp.14025. Epub 2020 Feb 19.

Abstract

PURPOSE

To measure ionization chamber dose response as a function of the angle between magnetic field direction and ionization chamber orientation in magnetic resonance-guided radiation therapy (MRgRT) system, and to evaluate angular dependence of magnetic field correction factor for reference dosimetry.

METHODS

Measurements were performed on an Elekta MR-linac that integrates a 1.5-T Philips MRI and a 7-MV FFF photon beam accelerator. The response of four reference class chambers (Exradin-A19, A1SL, IBA FC65-G, and CC13, paired with a PTW UE electrometer) was studied. An in-house built MR-compatible water tank and an accompanying cylindrical insert that allowed chamber rotation around the cylinder's axis was used. The EPID onboard imaging was used to center chamber at the MR-linac isocenter (143.5 cm, SAD), as well as to verify position at each datapoint.

RESULTS

A clear angular dependence of dose response for all chambers has been measured. The most significant effect of magnetic field on relative chamber response in the presence of magnetic field was observed in the orientation when chamber axis is perpendicular to the direction of magnetic field with the tip pointing in the same direction as Lorentz force. This effect is more pronounced for larger volume chambers; the maximum relative variation in the chamber response (between the setup described above and the one where chamber and magnetic field are parallel) is a 5.3% and 4.6% increase for A19 and FC65-G, respectively, and only 2.0% and 1.9% for smaller volume A1SL and CC13 chamber, respectively. We measured the absolute magnitude of the magnetic field correction factor for the Exradin-A19, A1SL, IBA FC65-G, and CC13 to be 0.938 ± 1.13%, 0.968 ± 0.99%, 0.950 ± 1.13%, and 0.975 ± 1.13%, respectively. The values are for perpendicular orientation of the chamber relative to magnetic field and parallel to the Lorentz force.

CONCLUSIONS

Experimental measurements carried out in this study have verified the optimal orientation of ionization chamber in terms of minimizing effect of magnetic field on the chamber dose response. This study provides a detailed high-resolution measurement of absolute values for four reference class chambers as a function of the angle between ionization chamber's central axis and the direction of strong magnetic field over a full 360° rotation. The experimental results of this study can further be used for optimization of the actual sensitive volume of the chamber (and analysis of dead volume) in future Monte Carlo chamber simulations in the presence of strong magnetic fields. In addition, it will provide some necessary data for future reference dosimetry protocols for MR-linac.

摘要

目的

测量磁共振引导放射治疗(MRgRT)系统中磁场方向与电离室方向之间的角度对电离室剂量响应的影响,并评估参考剂量学中磁场校正因子的角度依赖性。

方法

在 Elekta MR-linac 上进行了测量,该系统集成了 1.5-T Philips MRI 和 7-MV FFF 光子束加速器。研究了四个参考级电离室(Exradin-A19、A1SL、IBA FC65-G 和 CC13,与 PTW UE 静电计配对)的响应。使用了内部制造的 MR 兼容水箱和配套的圆柱形插件,允许电离室绕圆柱轴旋转。EPID 机载成像用于将电离室中心定位在 MR-linac 等中心(143.5 cm,SAD),并验证每个数据点的位置。

结果

已经测量到所有电离室剂量响应的明显角度依赖性。在存在磁场的情况下,磁场对相对电离室响应的影响最大,这种影响在电离室轴垂直于磁场方向且尖端指向洛伦兹力方向的方向上最为明显。对于较大体积的电离室,这种效应更为明显;在上述设置和磁场与电离室平行的设置之间,电离室响应的最大相对变化分别为 A19 和 FC65-G 的 5.3%和 4.6%增加,而较小体积的 A1SL 和 CC13 电离室仅为 2.0%和 1.9%。我们测量到 Exradin-A19、A1SL、IBA FC65-G 和 CC13 的磁场校正因子的绝对值分别为 0.938±1.13%、0.968±0.99%、0.950±1.13%和 0.975±1.13%,分别为 0.938±1.13%、0.968±0.99%、0.950±1.13%和 0.975±1.13%。这些值是在电离室相对于磁场垂直且平行于洛伦兹力的情况下测量的。

结论

本研究中的实验测量验证了在最小化磁场对电离室剂量响应影响方面,电离室的最佳取向。本研究提供了四个参考级电离室的绝对值的详细高分辨率测量值,作为电离室中心轴与强磁场方向之间的角度的函数,在 360°全旋转范围内。本研究的实验结果可进一步用于优化未来强磁场下实际电离室灵敏体积(和死区体积分析)的蒙特卡罗电离室模拟。此外,它将为未来的 MR-linac 参考剂量学协议提供一些必要的数据。

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