Department of Physics, Northern Illinois University, DeKalb, IL 60115, USA.
Phys Med Biol. 2010 Dec 7;55(23):7081-96. doi: 10.1088/0031-9155/55/23/S09. Epub 2010 Nov 12.
All particle beam scanning systems are subject to dose delivery errors due to errors in position, energy and intensity of the delivered beam. In addition, finite scan speeds, beam spill non-uniformities, and delays in detector, detector electronics and magnet responses will all contribute errors in delivery. In this paper, we present dose errors for an 8 × 10 × 8 cm(3) target of uniform water equivalent density with 8 cm spread out Bragg peak and a prescribed dose of 2 Gy. Lower doses are also analyzed and presented later in the paper. Beam energy errors and errors due to limitations of scanning system hardware have been included in the analysis. By using Gaussian shaped pencil beams derived from measurements in the research room of the James M Slater Proton Treatment and Research Center at Loma Linda, CA and executing treatment simulations multiple times, statistical dose errors have been calculated in each 2.5 mm cubic voxel in the target. These errors were calculated by delivering multiple treatments to the same volume and calculating the rms variation in delivered dose at each voxel in the target. The variations in dose were the result of random beam delivery errors such as proton energy, spot position and intensity fluctuations. The results show that with reasonable assumptions of random beam delivery errors, the spot scanning technique yielded an rms dose error in each voxel less than 2% or 3% of the 2 Gy prescribed dose. These calculated errors are within acceptable clinical limits for radiation therapy.
所有的粒子束扫描系统都可能由于束流的位置、能量和强度的误差而导致剂量传递误差。此外,有限的扫描速度、束流溢出不均匀性以及探测器、探测器电子学和磁体响应的延迟,都会导致剂量传递误差。在本文中,我们针对一个 8×10×8cm³的均匀水等效密度目标,其 8cm 处的布喇格峰展宽,规定剂量为 2Gy,分析了剂量误差。本文稍后还分析并给出了较低剂量的情况。在分析中包括了束流能量误差和扫描系统硬件限制引起的误差。通过使用在加利福尼亚州洛马林达詹姆斯·M·斯莱特质子治疗和研究中心的研究室中进行测量得到的高斯形状的铅笔束,并多次执行治疗模拟,计算了目标中每个 2.5mm³立方体素中的统计剂量误差。这些误差是通过对同一体积进行多次治疗并计算目标中每个体素的剂量分布的均方根变化来计算的。剂量的变化是由于质子能量、光斑位置和强度波动等随机束流传递误差引起的。结果表明,在合理假设随机束流传递误差的情况下,点扫描技术在每个体素中的剂量误差均方根小于规定剂量的 2Gy 的 2%或 3%。这些计算出的误差在放射治疗的可接受临床范围内。