Medical Physics Division, Department of Oncology, University of Alberta, 11560 University Avenue, Edmonton, Alberta, T6G 1Z2, Canada.
Department of Physics, University of Alberta, 11322 - 89 Avenue, Edmonton, Alberta, T6G 2G7, Canada.
Med Phys. 2017 Jun;44(6):2124-2131. doi: 10.1002/mp.12260. Epub 2017 May 12.
To modify a previously designed, short, 10 MV linac waveguide, so that it can produce any energy from 4 to 10 MV. The modified waveguide is designed to be a drop-in replacement for the 6 MV waveguide used in the author's current linear accelerator-magnetic resonance imager (Linac-MR).
Using our group's previously designed short 10 MV linac as a starting point, the port was moved to the fourth cavity, the shift to the first coupling cavity was removed and a tuning cylinder added to the first coupling cavity. Each cavity was retuned using finite element method (FEM) simulations to resonate at the desired frequency. FEM simulations were used to determine the RF field distributions for various tuning cylinder depths, and electron trajectories were computed using a particle-in-cell model to determine the required RF power level and tuning cylinder depth to produce electron energy distributions for 4, 6, 8, and 10 MV photon beams. Monte Carlo simulations were then used to compare the depth dose profiles with those produced by published electron beam characteristics for Varian linacs.
For each desired photon energy, the electron beam energy was within 0.5% of the target mean energy, the depth of maximum dose was within 1.5 mm of that produced by the Varian linac, and the ratio of dose at 10 cm depth to 20 cm depth was within 1%.
A new 27.5 cm linear accelerator waveguide design capable of producing any photon energy between 4 and 10 MV has been simulated, however coupling port design and the implications of increased electron beam current at 10 MV remain to be investigated. For the specific cases of 4, 6, and 10 MV, this linac produces depth dose profiles similar to those produced by published spectra for Varian linacs.
对之前设计的短款 10MV 直线加速器波导进行修改,使其能够产生 4 至 10MV 的任意能量。该修改后的波导旨在替代作者当前线性加速器磁共振成像仪(Linac-MR)中使用的 6MV 波导。
使用我们小组之前设计的短款 10MV 直线加速器作为起点,将端口移至第四腔,移除到第一耦合腔的移动,并在第一耦合腔中添加调谐圆柱。使用有限元方法(FEM)模拟对每个腔进行重新调谐,以在所需频率下产生共振。使用 FEM 模拟来确定各种调谐圆柱深度的射频场分布,并使用粒子在单元格模型计算电子轨迹,以确定产生 4、6、8 和 10MV 光子束的电子能量分布所需的射频功率水平和调谐圆柱深度。然后使用蒙特卡罗模拟将深度剂量分布与瓦里安直线加速器公布的电子束特性产生的深度剂量分布进行比较。
对于每个所需的光子能量,电子束能量在目标平均能量的 0.5%以内,最大剂量深度在瓦里安直线加速器产生的剂量深度的 1.5mm 以内,并且 10cm 深度处的剂量与 20cm 深度处的剂量之比在 1%以内。
已经模拟了一种新的 27.5cm 直线加速器波导设计,能够产生 4 至 10MV 之间的任意光子能量,但是耦合端口设计和 10MV 时电子束电流增加的影响仍有待研究。对于 4、6 和 10MV 的特定情况,该直线加速器产生的深度剂量分布与瓦里安直线加速器公布的光谱产生的深度剂量分布相似。