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Fast transit portal dosimetry using density-scaled layer modeling of aSi-based electronic portal imaging device and Monte Carlo method

机译:基于aSi的电子门成像设备的密度缩放层建模和Monte Carlo方法的快速传输门剂量

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Purpose: Fast and accurate transit portal dosimetry was investigated by developing a density-scaled layer model of electronic portal imaging device (EPID) and applying it to a clinical environment. Methods: The model was developed for fast Monte Carlo dose calculation. The model was validated through comparison with measurements of dose on EPID using first open beams of varying field sizes under a 20-cm-thick flat phantom. After this basic validation, the model was further tested by applying it to transit dosimetry and dose reconstruction that employed our predetermined dose-response-based algorithm developed earlier. The application employed clinical intensity-modulated beams irradiated on a Rando phantom. The clinical beams were obtained through planning on pelvic regions of the Rando phantom simulating prostate and large pelvis intensity modulated radiation therapy. To enhance agreement between calculations and measurements of dose near penumbral regions, convolution conversion of acquired EPID images was alternatively used. In addition, thickness-dependent image-to-dose calibration factors were generated through measurements of image and calculations of dose in EPID through flat phantoms of various thicknesses. The factors were used to convert acquired images in EPID into dose. Results: For open beam measurements, the model showed agreement with measurements in dose difference better than 2 across open fields. For tests with a Rando phantom, the transit dosimetry measurements were compared with forwardly calculated doses in EPID showing gamma pass rates between 90.8 and 98.8 given 4.5 mm distance-to-agreement (DTA) and 3 dose difference (DD) for all individual beams tried in this study. The reconstructed dose in the phantom was compared with forwardly calculated doses showing pass rates between 93.3 and 100 in isocentric perpendicular planes to the beam direction given 3 mm DTA and 3 DD for all beams. On isocentric axial planes, the pass rates varied between 95.8 and 99.9 for all individual beams and they were 98.2 and 99.9 for the composite beams of the small and large pelvis cases, respectively. Three-dimensional gamma pass rates were 99.0 and 96.4 for the small and large pelvis cases, respectively. Conclusions: The layer model of EPID built for Monte Carlo calculations offered fast (less than 1 min) and accurate calculation for transit dosimety and dose reconstruction.
机译:目的:通过开发电子门成像设备(EPID)的密度缩放层模型并将其应用于临床环境,研究了快速准确的运输门剂量。方法:开发该模型用于快速蒙特卡洛剂量计算。通过与在20厘米厚的扁平体模下使用不同场大小的第一条开放光束在EPID上进行剂量测量进行比较,验证了该模型的有效性。经过此基本验证后,该模型通过将其应用于采用先前开发的基于预定剂量响应的算法的传输剂量法和剂量重建而进一步测试。该申请采用了照射在兰多体模上的临床强度调制光束。通过在Rando体模的盆腔区域进行规划以模拟前列腺和大骨盆强度调制放射治疗,可以获得临床射线。为了增强半影区域附近剂量的计算和测量之间的一致性,可替代地使用获取的EPID图像的卷积转换。另外,通过对图像进行测量并通过各种厚度的扁平体模计算EPID中的剂量,可以生成与厚度相关的图像到剂量校准因子。这些因素用于将EPID中的采集图像转换为剂量。结果:对于开放束测量,该模型显示出与跨开放区域的剂量差测量结果优于2一致。对于使用Rando体模的测试,将传输剂量学测量与EPID中的向前计算剂量进行比较,显示在给定的4.5 mm协议距离(DTA)和3个剂量差(DD)的情况下,所有尝试使用的电子束的伽玛通过率在90.8和98.8之间在这个研究中。将体模中的重建剂量与向前计算的剂量进行比较,该剂量显示出在给定3 mm DTA和3 DD的所有射束的情况下,垂直于射束方向的等心垂直平面中的通过率在93.3和100之间。在等心轴平面上,所有单个光束的通过率在95.8和99.9之间变化,而小型和大型骨盆情况下的复合光束的通过率分别为98.2和99.9。小型和大型骨盆病例的三维伽玛通过率分别为99.0和96.4。结论:建立用于蒙特卡洛计算的EPID层模型可为运输剂量和剂量重建提供快速(不到1分钟)且准确的计算。

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