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斯坦福式与旋转技术在全身电子束照射疗法(TSET)中的皮肤剂量分布。

Skin dose distributions between Stanford and rotational techniques in total skin electron therapy (TSET).

机构信息

Department of Radiation Oncology, Vanderbilt University School of Medicine, Nashville, Tennessee, USA.

Department of Therapeutic Radiology, Yale University School of Medicine, New Haven, Connecticut, USA.

出版信息

Med Phys. 2022 Oct;49(10):6646-6653. doi: 10.1002/mp.15907. Epub 2022 Aug 23.

Abstract

PURPOSE

Total skin electron therapy (TSET) has proven to be one of the most effective treatments for advanced-stage cutaneous T-cell lymphoma. Two most used techniques are the Stanford six-field and rotational techniques. This study compares patient skin dose distributions as a function of depth between these two techniques.

METHODS

The EGSnrc system was used to simulate electron beams and calculate patient dose distributions. The calculations assumed the same patient standing on a platform, and the patient's different postures were ignored for the Stanford technique in the comparison of dose distributions. The skin doses were analyzed as a function of skin depth-dose coverage and evaluated using dose-volume-histograms (DVH). The comparisons were performed in three realistic clinical settings in which dual-field were used for patients treated at extended distances of 316 and 500 cm, and a single field was used at 700 cm. In all cases the realistic patient treatment beam delivery geometry was simulated.

RESULTS

Although small dose differences were observed in some local areas, no clinically significant differences were found in the patient 3D dose distributions between the Stanford and rotational techniques. Virtually the same DVH curves between two the techniques were observed for mean dose to skin depth of 0-5, 5-10, and 10-15 mm from the skin surface, respectively. It is found that the skin depth dose coverage is 2 mm shallower for patient treatment at 500 cm compared to at 316 cm due to the additional air attenuation. However, very similar dose coverage and uniformity can be achieved at these two different extended treatment distances by adjusting the thickness of acrylic scatter plate. Adequate thickness of a scattering plate improves the skin dose uniformity.

CONCLUSION

Both the Stanford and rotational techniques deliver very similar skin dose coverage in DVH plots, and only small differences are seen in local areas. It is worth to emphasize that the DVH is a graphical representation of the distribution of dose within a structure, and it does not contain spatial information. Therefore, comparison of entire skin dose using DVH may mask some variations at different locations of the surface area. In addition, the comparison did not consider different patient postures of the Stanford technique. Including the different patient postures in the calculation may affect the result of doses to the limbs.

摘要

目的

全身电子疗法(TSET)已被证明是治疗晚期皮肤 T 细胞淋巴瘤最有效的方法之一。两种最常用的技术是斯坦福六野和旋转技术。本研究比较了这两种技术的患者皮肤剂量分布与深度的关系。

方法

使用 EGSnrc 系统模拟电子束并计算患者的剂量分布。计算中假设患者站在同一个平台上,并且在比较剂量分布时忽略了斯坦福技术中患者不同姿势的影响。分析了皮肤剂量作为皮肤深度剂量覆盖的函数,并使用剂量-体积直方图(DVH)进行了评估。在三个实际临床环境中进行了比较,其中双野用于治疗距离为 316 和 500 cm 的患者,单野用于治疗距离为 700 cm 的患者。在所有情况下,都模拟了实际患者的治疗束传输几何形状。

结果

尽管在一些局部区域观察到了小的剂量差异,但在斯坦福技术和旋转技术之间,患者的三维剂量分布没有发现临床意义上的差异。对于距皮肤表面 0-5、5-10 和 10-15 mm 的皮肤深度的平均剂量,两种技术之间几乎观察到相同的 DVH 曲线。发现在 500 cm 处治疗的患者由于额外的空气衰减,皮肤深度剂量覆盖比在 316 cm 处浅 2mm。然而,通过调整有机玻璃散射板的厚度,可以在这两个不同的延伸治疗距离实现非常相似的剂量覆盖和均匀性。散射板的足够厚度可以提高皮肤剂量的均匀性。

结论

斯坦福技术和旋转技术在 DVH 图中都能提供非常相似的皮肤剂量覆盖,并且仅在局部区域观察到很小的差异。值得强调的是,DVH 是结构内剂量分布的图形表示,它不包含空间信息。因此,使用 DVH 比较整个皮肤剂量可能会掩盖表面不同位置的一些变化。此外,比较未考虑斯坦福技术的不同患者姿势。在计算中包括斯坦福技术的不同患者姿势可能会影响四肢的剂量结果。

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