CBCT acquired during beam delivery

  • 文章类型: Journal Article
    目的:为了精确的肺部立体定向放射治疗,应在束传递过程中获取目标位置。我们旨在在相位门控条件下在光束辐照(辐照内成像)期间进行千伏(kV)成像,并评估其性能。
    方法:使用Catphan504和QUASAR呼吸运动体模评估图像质量和目标可检测性,分别。使用了TrueBeamSTx直线加速器和开发者模式。成像参数为125kVp和1.2mAs/投影。使用平坦的兆伏(MV)X射线束能量6、10和15MV以及未平坦的束能量6和10MV,场大小为5×5和15×15cm2,并且具有各种帧速率,用于照射内成像。此外,使用量子幻影,在调强计划实施期间进行照射内成像.插入杆的CT数的均方根误差(RMSE),图像噪声,视觉评估,和对比噪声比(CNR)进行了评估。
    结果:门控条件下辐照内锥形束计算机断层扫描(CBCT)图像的RMSE为50-230Hounsfield单位(HU)(静态<30HU)。门控条件下照射内CBCT图像的噪声为15-35HU,而标准CBCT图像为8.8-27.2HU。较低的帧速率表现出较大的RMSE和噪声;然而,迭代重建算法(IR)在改善这些值方面是有效的。具有IR的大约7fps显示出没有IR的15fps的等效CNR。目标在所有门控照射内CBCT图像上可见。
    结论:需要改善图像质量;然而,照射内CBCT图像显示良好的视觉目标检测。
    OBJECTIVE: Target positions should be acquired during beam delivery for accurate lung stereotactic body radiotherapy. We aimed to perform kilovoltage (kV) imaging during beam irradiation (intra-irradiation imaging) under phase-gated conditions and evaluate its performance.
    METHODS: Catphan 504 and QUASAR respiratory motion phantoms were used to evaluate image quality and target detectability, respectively. TrueBeam STx linac and the Developer Mode was used. The imaging parameters were 125 kVp and 1.2 mAs/projection. Flattened megavoltage (MV) X-ray beam energies 6, 10 and 15 MV and un-flattened beam energies 6 and 10 MV were used with field sizes of 5 × 5 and 15 × 15 cm2 and various frame rates for intra-irradiation imaging. In addition, using a QUASAR phantom, intra-irradiation imaging was performed during intensity-modulated plan delivery. The root-mean-square error (RMSE) of the CT-number for the inserted rods, image noise, visual assessment, and contrast-to-noise ratio (CNR) were evaluated.
    RESULTS: The RMSEs of intra-irradiation cone-beam computed tomography (CBCT) images under gated conditions were 50-230 Hounsfield Unit (HU) (static < 30 HU). The noise of the intra-irradiation CBCT images under gated conditions was 15-35 HU, whereas that of the standard CBCT images was 8.8-27.2 HU. Lower frame rates exhibited large RMSEs and noise; however, the iterative reconstruction algorithm (IR) was effective at improving these values. Approximately 7 fps with the IR showed an equivalent CNR of 15 fps without the IR. The target was visible on all the gated intra-irradiation CBCT images.
    CONCLUSIONS: Several image quality improvements are required; however, intra-irradiated CBCT images showed good visual target detection.
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  • 文章类型: Journal Article
    目的:在脊柱立体定向身体放射治疗中,必须从批准的患者设置中量化分数内六自由度(6DoF)残余误差或运动,以进行精确的束输送。然而,先前报告的错误未在光束传递过程中获得。因此,我们的目的是量化的6DoF残余误差和运动期间使用并发锥形束计算机断层扫描(CBCT)成像技术的弧形束传输,照射内CBCT。
    方法:连续15名患者,19个不同治疗地点的计划,分析了199张CBCT图像。使用ExacTrac系统进行预照射CBCT以验证从初始患者设置的偏移。在通过两个或三个共面全弧旋转的光束传递过程中,同时进行CBCT成像。随后,重建了照射内CBCT图像。基于骨骼,将辐照前和辐照内CBCT图像与计划CT图像进行严格配准,以量化6DoF残余误差。
    结果:使用辐照前和辐照内CBCT量化的6DoF残余误差在2.0mm/2.0°以内,除了一个测量。预照射CBCT到最后一次电弧束递送结束后的平均经过时间(平均值±标准偏差[min:sec])为6:08±1:25和7:54±2:14,分别。几个方向的残余误差的均方根显示出显着差异;但是,它们在1.0毫米/1.0°以内。与时间相关的分析表明,剩余误差随着时间的流逝而增加。
    结论:与使用前,梁间,和6DoF后图像指导,可以在标准治疗时隙内获取。
    OBJECTIVE: Quantifying intra-fractional six-degree-of-freedom (6DoF) residual errors or motion from approved patient setups is necessary for accurate beam delivery in spine stereotactic body radiotherapy. However, previously reported errors were not acquired during beam delivery. Therefore, we aimed to quantify the 6DoF residual errors and motions during arc beam delivery using a concurrent cone-beam computed tomography (CBCT) imaging technique, intra-irradiation CBCT.
    METHODS: Consecutive 15 patients, 19 plans for various treatment sites, and 199 CBCT images were analyzed. Pre-irradiation CBCT was performed to verify shifts from the initial patient setup using the ExacTrac system. During beam delivery by two or three co-planar full-arc rotations, CBCT imaging was performed concurrently. Subsequently, an intra-irradiation CBCT image was reconstructed. Pre- and intra-irradiation CBCT images were rigidly registered to a planning CT image based on the bone to quantify 6DoF residual errors.
    RESULTS: 6DoF residual errors quantified using pre- and intra-irradiation CBCTs were within 2.0 mm/2.0°, except for one measurement. The mean elapsed time (mean ± standard deviation [min:sec]) after pre-irradiation CBCT to the end of the last arc beam delivery was 6:08 ± 1:25 and 7:54 ± 2:14 for the 2- and 3-arc plans, respectively. Root mean squares of residual errors for several directions showed significant differences; however, they were within 1.0 mm/1.0°. Time-dependent analysis revealed that the residual errors tended to increase with elapsed time.
    CONCLUSIONS: The errors represent the optimal intra-fractional error compared with those acquired using the pre-, inter-beam, and post-6DoF image guidance and can be acquired within a standard treatment timeslot.
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