Baghani Hamid Reza, Andreoli Stefano, Robatjazi Mostafa
Physics Department, Hakim Sabzevari University, Sabzevar, Iran.
Fisica Scanitaria, ASST Papa Giovanni XXIII, Bergamo, Italy.
Phys Eng Sci Med. 2023 Mar;46(1):185-195. doi: 10.1007/s13246-022-01209-0. Epub 2023 Jan 3.
Ionometric electron dosimetry inside water-equivalent plastic phantoms demands special considerations including determination of depth scaling and fluence scaling factors (c and h) to shift from in-phantom measurements to those relevant to water. This study evaluates these scaling factors for RW3 slab phantom and also introduces a new coefficient, k(RW3), for direct conversion from RW3 measurements to water without involving scaling factors. The RW3 solid phantom developed by the PTW Company was used and the corresponding scaling factors including c, h, and k(RW3) were measured for conventional electron energies of 4, 6, 9, 12, and 16 MeV. Separate measurements were performed in water and the RW3 slab phantom using the Advanced Markus chamber. The validity of the reported scaling factors was confirmed by comparing the direct and indirect percentage depth dose (PDD) measurements in water and in the RW3 phantom. The c values for the RW3 phantom were respectively equal to 0.915, 0.927, 0.934, 0.937, and 0.937 for 4, 6, 9, 12, and 16 MeV electron energies. The h and k(RW3) values were dependent on the depth of investigation and electron energy. Application of the c-h factors and k(RW3) coefficients to measured data inside the RW3 can reliably reproduce the measured PDD curves in water. The mean difference between the PDDs measured directly and indirectly in water and in the RW3 phantom was less than 1.2% in both approaches for PDD conversion (c-h coupling and the use of k(RW3)). The measured scaling factors and k(RW3) coefficients are sufficiently relevant to mimic water-based dosimetry results through indirect measurements inside the RW3 slab phantom. Nevertheless, employing k(RW3) is more straightforward than the c-h approach because it does not involve scaling and it is also less time-consuming.
在水等效塑料模体内部进行离子测量电子剂量测定需要特殊考虑,包括确定深度缩放因子和注量缩放因子(c和h),以便从模体内测量转换为与水相关的测量。本研究评估了RW3平板模体的这些缩放因子,并引入了一个新系数k(RW3),用于直接从RW3测量转换为水的测量,而无需涉及缩放因子。使用了PTW公司开发的RW3固体模体,并针对4、6、9、12和16 MeV的常规电子能量测量了相应的缩放因子,包括c、h和k(RW3)。使用高级马克斯电离室在水和RW3平板模体中分别进行测量。通过比较在水和RW3模体中的直接和间接百分深度剂量(PDD)测量,证实了所报告缩放因子的有效性。对于4、6、9、12和16 MeV的电子能量,RW3模体的c值分别等于0.915、0.927、0.934、0.937和0.937。h和k(RW3)值取决于研究深度和电子能量。将c-h因子和k(RW3)系数应用于RW3内部的测量数据,可以可靠地重现水中测量的PDD曲线。在PDD转换的两种方法(c-h耦合和使用k(RW3))中,在水和RW3模体中直接和间接测量的PDD之间的平均差异均小于1.2%。所测量的缩放因子和k(RW3)系数与通过RW3平板模体内部的间接测量来模拟水基剂量测定结果具有足够的相关性。然而,使用k(RW3)比c-h方法更直接,因为它不涉及缩放,而且也更省时。