Division of Radiation Oncology, National Cancer Centre Singapore, Singapore.
Oncology Academic Clinical Programme, Duke-NUS Medical School, Singapore.
Phys Med Biol. 2023 Nov 6;68(22). doi: 10.1088/1361-6560/ad0536.
. Dispersion in an accelerator quantifies the deviation of the proton trajectory when there is a momentum deviation. We present for the first time a safe method of measuring dispersion in the clinic, using a scintillator detector and the momentum deviations within a spill. This is an important accelerator quantity as we found that this is the reason behind the large dose fluctuation in our absolute dosimetry measurement.. Dispersions are measured for nine energies in a Hitachi ProBeat system at three locations (isocenter and at two profile monitors) and at two gantry angles (0 and 90 degrees) by first measuring the spot position and momentum drift within a spill. The spot position drift is measured by the XRV-4000 at the isocenter, and by the two profile monitors located at 0.57 and 2.27 m from the isocenter. The momentum drift is calculated from the intra-spill range drift which is measured using the Ranger accessory. The dispersion at isocenter and its gradient are calculated using the weighted least square regression on the measured dispersions at the three locations. A constraint is formulated on the dispersion and its gradient to ensure minimal intra-spill spot position deviation around the isocenter.. The measured intra-spill range and spot positional drift at isocenter are less than0.25mmand0.7mmrespectively. The momentum spread calculated from the range drift are less than 0.08%. The dispersion at the isocenter ranged from0.50to4.30mand the zero-crossing happens upstream of isocenter for all energies. 2 of the 9 energies (168.0 and 187.5 MeV) violated the constraint and has an intra-spill spot positional deviation greater than1.0within5cmfrom the isocenter.. This measurement is recommended as part of commissioning and annual quality assurance for accelerator monitoring and to ensure intra-spill spot deviations remain low.
在加速器中,弥散度量化了质子轨迹在动量偏差时的偏离程度。我们首次提出了一种在临床环境中测量弥散度的安全方法,使用闪烁体探测器和束流间隔内的动量偏差。这是一个重要的加速器参数,因为我们发现这是我们在绝对剂量测量中剂量波动较大的原因。在日立 ProBeat 系统中,我们在三个位置(等中心和两个轮廓监视器)和两个旋转架角度(0 度和 90 度)下测量了九个能量的弥散度,首先测量了束流间隔内的光斑位置和动量漂移。在等中心,XRV-4000 测量光斑位置漂移,在距等中心 0.57 和 2.27 米处的两个轮廓监视器测量位置漂移。通过 Ranger 附件测量的束内间隔漂移来计算动量漂移。通过对三个位置测量的弥散度进行加权最小二乘回归,计算等中心处的弥散度及其梯度。对弥散度及其梯度进行约束,以确保等中心周围束内光斑位置的偏差最小。在等中心处测量的束内间隔和光斑位置漂移小于 0.25mm 和 0.7mm。从漂移计算得出的动量分布小于 0.08%。等中心处的弥散度在 0.50 到 4.30m 之间,所有能量的零交叉点都在等中心的上游。在 9 个能量中,有 2 个(168.0 和 187.5 MeV)违反了约束条件,在距等中心 5cm 范围内的束内光斑位置偏差大于 1.0。建议在加速器监测的调试和年度质量保证中进行这项测量,以确保束内光斑偏差保持在较低水平。