Department of Medical Physics, Faculty of Medical Sciences, Tarbiat Modares University, Tehran, Iran.
Biomedical Engineering and Medical Physics Department, School of Medicine, Shahid Beheshti University of Medical Sciences, Tehran, Iran.
Med Phys. 2023 Jun;50(6):3701-3718. doi: 10.1002/mp.16259. Epub 2023 Mar 15.
We investigated the design of a prompt gamma camera for real-time dose delivery verification and the partial mitigation of range uncertainties.
A slit slat (SS) camera was optimized using the trade-off between the signal-to-noise ratio and spatial resolution. Then, using the GATE Monte Carlo package, the camera performances were estimated by means of target shifts, beam position quantification, changing the camera distance from the beam, and air cavity inserting. A homogeneous PMMA phantom and the air gaps induced PMMA phantom were used. The air gaps ranged from 5 mm to 30 mm by 5 mm increments were positioned in the middle of the beam range. To reduce the simulation time, phase space scoring was used. The batch method with five realizations was used for stochastic error calculations.
The system's detection efficiency was PGs/proton) for a 10 × 20 cm detector (source-to-collimator distance = 15.0 cm). Axial and transaxial resolutions were 23 mm and 18 mm, respectively. The SS camera estimated the range as 69.0 ± 3.4 (relative stochastic error 1-sigma is 5%) and 67.6 ± 1.8 mm (2.6%) for the real range of 67.0 mm for 10 and 10 protons of 100 MeV, respectively. Considering 160 MeV, these values are 155.5 ± 3.1 (2%) and 152.2 ± 2.0 mm (1.3%) for the real range of 152.0 mm for 10 and 10 protons, respectively. Considering phantom shift, for a 100 MeV beam, the precision of the quantification (1-sigma) in the axial and lateral phantom shift estimation is 2.6 mm and 1 mm, respectively. Accordingly, the axial and lateral quantification precisions were 1.3 mm and 1 mm for a 160 MeV beam, respectively. Furthermore, the quantification of an air gap formulated as , where and gap are the estimated and real air gap, respectively. The precision of the air gap quantification is 1.6 mm (1 sigma). Moreover, 2D PG images show the trajectory of the proton beam through the phantom.
The proposed slit-slat imaging systems can potentially provide a real-time, in-vivo, and non-invasive treatment monitoring method for proton therapy.
我们研究了一种实时剂量验证和部分缓解射程不确定性的prompt gamma 相机的设计。
采用信号噪声比和空间分辨率之间的折衷优化了狭缝片(SS)相机。然后,使用 GATE 蒙特卡罗软件包,通过目标移动、光束位置量化、改变相机与光束的距离以及插入空气腔来估计相机性能。使用均匀的 PMMA 体模和诱导 PMMA 体模中的空气间隙。空气间隙范围为 5 毫米至 30 毫米,增量为 5 毫米,位于光束范围内的中间。为了减少模拟时间,使用了相空间评分。采用五次实现的批处理方法进行随机误差计算。
系统的探测效率为 PGs/质子),用于 10×20 cm 探测器(源至准直器距离= 15.0 cm)。轴向和横向分辨率分别为 23mm 和 18mm。SS 相机分别估计 10 和 10 个 100 MeV 质子的真实射程为 67.0mm 的 69.0±3.4(相对随机误差 1-sigma 为 5%)和 67.6±1.8mm(2.6%)。对于 160 MeV,这些值分别为 155.5±3.1(2%)和 152.2±2.0mm(1.3%),对于 152.0mm 的真实射程为 10 和 10 个 160 MeV 质子。考虑到体模移位,对于 100 MeV 束,轴向和横向体模移位估计的定量精度(1-sigma)分别为 2.6mm 和 1mm。因此,对于 160 MeV 束,轴向和横向定量精度分别为 1.3mm 和 1mm。此外,空气间隙的定量公式为 ,其中 和 gap 分别是估计的和实际的空气间隙。空气间隙定量的精度为 1.6mm(1 sigma)。此外,2D PG 图像显示了质子束通过体模的轨迹。
所提出的狭缝片成像系统有可能为质子治疗提供一种实时、体内和非侵入性的治疗监测方法。