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arXiv 1708.07538physics.med-ph
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用Varian TrueBeam光子相空间作为粒子源的蒙特卡罗剂量计算中潜在方差的评估

Evaluation of latent variances in Monte Carlo dose calculations with Varian TrueBeam photon phase-spaces used as a particle source

Eyad Alhakeem, Sergei Zavgorodni

摘要:

目的:评价开放10 x 10 $cm^2$和小视野的TrueBeam光子相空间文件(PSF)的潜在方差(LV)。方法:利用BEAMnrc/DOSXYZnrc将Varian相空间文件(PSFA)中的粒子通过二级准直器进行传输。将输送的颗粒刻划到位于钳口下方的另一个相空间(PSFB)中,或进一步输送通过锥形准直器并在正下方刻划,形成PSFC。在直径为0.13、0.25、0.35、1.0、1.2、1.5和4cm的锥体下,对6MV-FFF、6MV、10MV-FFF、10MV和15MV射束的PFSB进行评分,并对6MV射束的PSFC进行评分。PSFB和PSFC被输送到水模体中,颗粒循环数范围为10至1000。对于10 × 10 $cm^2$射野,使用0.5 × 0.5 × 0.5 cm ^3体素对剂量进行评分,而对于用小锥准直的射束,使用0.1 × 0.1 × 0.5 cm ^3体素对剂量进行评分。对于直径为0.25 cm的小型锥形准直6MV射束,体模体素尺寸变化为0.02x0.02x0.5cm^3、0.05x0.05x0.5cm^3和0.1x0.1x0.5cm^3。根据Sempau等人对所有病例的剂量差异进行评分,并对LV进行评价。结果:对于10 x 10 cm ^2射野,计算的LV在体模表面最大,并随深度降低,直至在5 cm深度达到平台。在10cm深度处,6MV-FFF、6MV、10MV-FFF、10MV和15MV能量的LV分别为0.54%、0.96%、0.35%、0.69%和0.57%。对于6MV相空间准直器,在1.5cm深度处,用直径为0.13、0.25、0.35、1.0cm的锥进行准直,计算的LV分别为75.6%、25.4%、17.6%和8.0%。在0.02x0.02x0.5cm^3、0.05x0.05x0.5cm^3和0.1x0.1x0.5cm^3体素中,0.25 cm锥形准直6MV射束的计算LV分别为61.2%、40.7%和22.5%。结论:单个PSF可用于在开放的10 × 10cm^2场MC模拟中实现亚百分比的潜在方差,而对于小SRS场,必须对更多的PSF求和。

英文摘要:

Purpose: To evaluate the latent variance (LV) of TrueBeam photon phase-space files (PSF) for open 10x10$cm^2$ and small fields. Methods: BEAMnrc/DOSXYZnrc was used to transport particles from Varian phase-space files (PSFA) through the secondary collimators. Transported particles were scored into another phase-space located under the jaws (PSFB), or transported further through the cone collimators and scored straight below, forming PSFC. PFSB were scored for 6MV-FFF, 6MV, 10MV-FFF, 10MV and 15MV beams with 10x10$cm^2$ field size, and PSFC were scored for 6MV beam under cones of 0.13, 0.25, 0.35, 1.0, 1.2, 1.5 and 4cm diameter. PSFB and PSFC were transported into a water phantom with particle recycling number ranging from 10 to 1000. For 10x10$cm^2$ fields 0.5x0.5x0.5cm^3 voxels were used to score the dose, whereas the dose was scored in 0.1x0.1x0.5cm^3 voxels for beams collimated with small cones. For small 0.25cm diameter cone-collimated 6MV beam, phantom voxel size varied as 0.02x0.02x0.5cm^3, 0.05x0.05x0.5cm^3 and 0.1x0.1x0.5cm^3. Dose variances were scored in all cases and LV evaluated as per Sempau et al. Results: For the 10x10cm^2 fields calculated LVs were greatest at the phantom surface and decreased with depth until reached a plateau at 5cm depth. LVs were 0.54%, 0.96%, 0.35%, 0.69% and 0.57% for the 6MV-FFF, 6MV, 10MV-FFF, 10MV and 15MV energies, respectively at 10cm depth. For the 6 MV phase-space collimated with cones of 0.13, 0.25, 0.35, 1.0cm diameter, the LVs calculated at 1.5cm depth were 75.6%, 25.4%, 17.6% and 8.0% respectively. Calculated LV for the 0.25cm cone-collimated 6MV beam were 61.2%, 40.7%, 22.5% in 0.02x0.02x0.5cm^3, 0.05x0.05x0.5cm^3 and 0.1x0.1x0.5cm^3 voxels respectively. Conclusion: Single PSF can be used to achieve sub-percent latent variance in open 10x10cm^2 field MC simulations, whereas more PSFs would have to be summed for small SRS fields.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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