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简化调强放射治疗验证中的 EPID 剂量学。

Simplifying EPID dosimetry for IMRT treatment verification.

机构信息

Department of Radiation Oncology, The Netherlands Cancer Institute-Antoni van Leeuwenhoek Hospital, Plesmanlaan 121, 1066 CX Amsterdam, The Netherlands.

出版信息

Med Phys. 2011 Feb;38(2):983-92. doi: 10.1118/1.3547714.

Abstract

PURPOSE

Electronic portal imaging devices (EPIDs) are increasingly used for IMRT dose verification, both pretreatment and in vivo. In this study, an earlier developed backprojection model has been modified to avoid the need for patient-specific transmission measurements and, consequently, leads to a faster procedure.

METHODS

Currently, the transmission, an essential ingredient of the backprojection model, is estimated from the ratio of EPID measurements with and without a phantom/patient in the beam. Thus, an additional irradiation to obtain "open images" under the same conditions as the actual phantom/patient irradiation is required. However, by calculating the transmission of the phantom/patient in the direction of the beam instead of using open images, this extra measurement can be avoided. This was achieved by using a model that includes the effect of beam hardening and off-axis dependence of the EPID response on photon beam spectral changes. The parameters in the model were empirically obtained by performing EPID measurements using polystyrene slab phantoms of different thickness in 6, 10, and 18 MV photon beams. A theoretical analysis to verify the sensitivity of the model with patient thickness changes was performed. The new model was finally applied for the analysis of EPID dose verification measurements of step-and-shoot IMRT treatments of head and neck, lung, breast, cervix, prostate, and rectum patients. All measurements were carried out using Elekta SL20i linear accelerators equipped with a hydrogenated amorphous silicon EPID, and the IMRT plans were made using PINNACLE software (Philips Medical Systems).

RESULTS

The results showed generally good agreement with the dose determined using the old model applying the measured transmission. The average differences between EPID-based in vivo dose at the isocenter determined using either the new model for transmission and its measured value were 2.6 +/- 3.1%, 0.2 +/- 3.1%, and 2.2 +/- 3.9% for 47 patients treated with 6, 10, and 18 MV IMRT beams, respectively. For the same group of patients, the differences in mean gamma analysis (3% maximum dose, 3 mm) were 0.16 +/- 0.26%, 0.21 +/- 0.24%, and 0.02 +/- 0.12%, respectively. For a subgroup of 11 patients, pretreatment verification was also performed, showing similar dose differences at the isocenter: -1.9 +/- 0.9%, -1.4 +/- 1.2%, and -0.4 +/- 2.4%, with somewhat lower mean gamma difference values: 0.01 +/- 0.09%, 0.01 +/- 0.07%, and -0.09 +/- 0.10%, respectively. Clinical implementation of the new model would save 450 h/yr spent in measurement of open images.

CONCLUSIONS

It can be concluded that calculating instead of measuring the transmission leads to differences in the isocenter dose generally smaller than 2% (2.6% for 6 MV photon beams for in vivo dose) and yielded only slightly higher gamma-evaluation parameter values in planes through the isocenter. Hence, the new model is suitable for clinical implementation and measurement of open images can be omitted.

摘要

目的

电子射野影像装置(EPID)越来越多地用于调强放疗剂量验证,包括治疗前和体内。在这项研究中,我们对之前开发的反向投影模型进行了修改,以避免对患者特定的透射测量的需求,从而使过程更快。

方法

目前,反向投影模型中的透射是通过比较有和没有射野内模体/患者的 EPID 测量值来估计的。因此,需要进行额外的照射以在与实际模体/患者照射相同的条件下获得“开放图像”。然而,通过计算射束方向上的模体/患者的透射,而不是使用开放图像,可以避免这种额外的测量。通过使用包括束硬化效应和 EPID 响应在光子束光谱变化的轴外依赖性的模型来实现这一点。通过使用不同厚度的聚苯乙烯平板模体在 6、10 和 18 MV 光子束中进行 EPID 测量,从经验上获得了模型中的参数。对模型的灵敏度进行了理论分析,以验证患者厚度变化。最后,新模型应用于头部和颈部、肺部、乳房、宫颈、前列腺和直肠患者的步进和射击调强放疗治疗的 EPID 剂量验证测量分析。所有测量均使用配备氢化非晶硅 EPID 的 Elekta SL20i 直线加速器进行,并使用 PINNACLE 软件(飞利浦医疗系统)制作 IMRT 计划。

结果

结果显示,与应用测量的透射值的旧模型确定的剂量相比,通常具有较好的一致性。对于用 6、10 和 18 MV IMRT 束治疗的 47 名患者,使用新模型进行透射测量的 EPID 体内剂量在等中心处的平均差异分别为 2.6% +/- 3.1%、0.2% +/- 3.1%和 2.2% +/- 3.9%。对于同一组患者,平均伽马分析(3%最大剂量,3 毫米)的差异分别为 0.16% +/- 0.26%、0.21% +/- 0.24%和 0.02% +/- 0.12%。对于 11 名患者的亚组,还进行了治疗前验证,等中心处的剂量差异相似:-1.9% +/- 0.9%、-1.4% +/- 1.2%和-0.4% +/- 2.4%,平均伽马差异值略低:0.01% +/- 0.09%、0.01% +/- 0.07%和-0.09% +/- 0.10%。新模型的临床应用将节省每年 450 小时的开放图像测量时间。

结论

可以得出结论,计算而不是测量透射会导致等中心剂量的差异通常小于 2%(对于 6 MV 光子束的体内剂量为 2.6%),并且在等中心平面上仅略微提高了伽马评估参数值。因此,新模型适用于临床应用,可以省略开放图像的测量。

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