Klein E E, Low D A, Purdy J A
Mallinckrodt Institute of Radiology, Washington University School of Medicine, St. Louis, MO, USA.
Int J Radiat Oncol Biol Phys. 1995 May 15;32(2):483-90. doi: 10.1016/0360-3016(94)00452-Q.
The optimization of clinical electron beams is a challenge to accelerator manufacturers. There are numerous variations and reports of scattering-foil and applicator configurations. The accelerator at our facility was recently updated with new foils and applicators. We conducted many dosimetric tests to critically evaluate dosimetric changes and their clinical effects.
The new dual foil systems are thicker and have shaped disks seated on the lower foils. The 12 MeV beam no longer shares a common foil used for 6 and 9 MeV. The applicators now have denser collimating plates, and Fiberglas no longer connects the plates. The new applicator set includes a rectangular 10 x 6 cm applicator that uses one photon jaw setting for all energies. After the electron beam energies were tuned to previous specifications (energy according to ionization depths, symmetry to +/- 2%, and flatness to +/- 6%), recommissioning took place. Electron beam output checks at various source-to-skin distances (SSD) were conducted for all energies and applicators. Computer-driven water scanning provided percent depth dose, profile, isodose, and Bremsstrahlung data. Surface doses, in-air electron dispersion, effective SSDs, and leakage were also measured. All results compared the previous and updated systems.
We found little change in relative percent depth doses for 100 cm SSD between the two systems. The differences in PDD due to increasing SSD, however, decreased with the updated system. Surface doses decreased in most cases, while Bremsstrahlung increased in all cases (typically by a factor of two). Beam uniformity indices increased significantly, while penumbra widths decreased. Diagonal profiles are now quite flat for large fields. For a 20 MeV beam, the 90% width along the diagonal axis for a 25 x 25 applicator at dmax depth has increased from 25 to 32 cm. There was little or no change in 'effective SSD' or in-air dispersion. Leakage outside the applicators was reduced by a factor of two to three. The flatness characteristics of the 10 x 6 cm applicator were poor in comparison to the improved flatness of the new square applicators.
The updated scattering foil-applicator electron beam system has yielded many dosimetric changes. Major improvements have been made in beam flatness and leakage. These positive changes have not been accompanied by any clinically significant dosimetric deficiencies.
临床电子束的优化对加速器制造商而言是一项挑战。散射箔和施源器配置存在众多变化及相关报告。我们机构的加速器最近更新了新的箔片和施源器。我们进行了许多剂量学测试,以严格评估剂量学变化及其临床效果。
新的双箔系统更厚,且在下部箔片上装有成型盘。12 MeV 电子束不再共用用于 6 MeV 和 9 MeV 的通用箔片。施源器现在具有更密集的准直板,并且玻璃纤维不再连接这些板。新的施源器套装包括一个 10×6 cm 的矩形施源器,它对所有能量均使用一种光子限束器设置。在将电子束能量调整到先前规格(根据电离深度确定能量,对称性达到±2%,平坦度达到±6%)之后,重新进行了调试。针对所有能量和施源器,在不同源皮距(SSD)下进行了电子束输出检查。计算机驱动的水扫描提供了百分深度剂量、剂量分布、等剂量线和轫致辐射数据。还测量了表面剂量、空气中电子散射、有效 SSD 和泄漏情况。所有结果均对先前系统和更新后的系统进行了比较。
我们发现,对于 100 cm SSD,两个系统之间的相对百分深度剂量变化不大。然而,随着 SSD 增加,更新后的系统中由于 SSD 增加导致的百分深度剂量差异减小。在大多数情况下,表面剂量降低,而在所有情况下轫致辐射均增加(通常增加一倍)。束流均匀性指数显著增加,而半值层宽度减小。对于大射野,对角剂量分布现在相当平坦。对于 20 MeV 电子束,在 dmax 深度处,25×25 施源器沿对角轴的 90%宽度已从 25 cm 增加到 32 cm。“有效 SSD”或空气中散射几乎没有变化。施源器外部的泄漏减少了两到三倍。与新方形施源器改善后的平坦度相比,10×6 cm 施源器的平坦度特性较差。
更新后的散射箔 - 施源器电子束系统产生了许多剂量学变化。在束流平坦度和泄漏方面有了重大改进。这些积极变化并未伴随任何临床上显著的剂量学缺陷。