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研究高剂量率(DQE)兆伏(MV)探测器联合千伏(kV)/兆伏锥形束 CT(CBCT)成像。

Investigation of combined kV/MV CBCT imaging with a high-DQE MV detector.

机构信息

Department of Physics and Astronomy, University of Victoria, 3800 Finnerty Rd, Victoria, BC, V8P 5C2, Canada.

Varian Medical Systems, 3120 Hansen Way, Palo Alto, CA, 94304, USA.

出版信息

Med Phys. 2019 Feb;46(2):563-575. doi: 10.1002/mp.13291. Epub 2018 Dec 6.

Abstract

PURPOSE

Combined kV-MV cone-beam tomography (CBCT) imaging has been proposed for two potentially important image-guided radiotherapy applications: (a) scan time reduction (STR) and (b) metal artifact reduction (MAR). However, the feasibility of these techniques has been in question due to the low detective quantum efficiencies (DQEs) of commercially available electronic portal imagers (EPIDs). The goal of the work was to test whether a prototype high DQE MV detector can be used to generate acceptable quality pretreatment CBCT images at acceptable dose levels.

METHODS

6MV and 100 kVp projection data were acquired on a Truebeam system (Varian, Palo Alto, CA). The MV data were acquired using a prototype EPID containing two scintillators (a) a standard copper-gadolinium oxysulfide (Cu-GOS) screen having a zero-frequency DQE (DQE(0)) value of 1.4%, and (b) a prototype-focused cadmium tungstate (CWO) pixelated "strip" with a DQE(0) = 22%. The kV data were acquired using the standard onboard imager (DQE(0) = 70%). The angular spacing of the MV projections was 0.81° and the source output was 0.03 MU/projection while the kV projections were acquired with an angular spacing of 0.4° at 0.3 mAs/projection. Image quality was evaluated using (a) an 18-cm diameter electron density phantom (CIRS, Norfolk, VA) with nine contrast inserts and (b) the resolution section of the 20-cm diameter Catphan phantom (The Phantom Laboratory, Greenwich, NY). For the MAR studies, two opposing CIRS phantom inserts were replaced by steel rods. The reconstruction methods were based on combining MV and kV data into one sinogram. The MAR reconstruction utilized mostly kV raw data with only those rays corrupted by metal requiring replacement with MV data (total absorbed dose = 0.7 cGy). For the STR study, projections from partially overlapping 105°kV and MV acquisitions were combined to create a complete dataset that could have been acquired in 18 sec (absorbed dose = 2.5 cGy). MV-only (4.3 cGy) and kV-only (0.3 cGy) images were also reconstructed.

RESULTS

The average signal-to-noise ratio (SNR) of the inserts in the MV-only CWO and GOS CIRS phantom images were 0.62× and 0.12× the SNR of the inserts in kV-only image, respectively. The limiting spatial resolutions in the MV-only GOS, MV-only CWO, and kV-only Catphan images were 3, 6, and 8 lp/cm, respectively. In the combined kV/CWO STR reconstruction, all contrast inserts were visible while only two were detectable in the kV/Cu-GOS image due to high levels of noise (average SNRs of kV/CWO and kV/GOS inserts were 0.97× and 0.18× the SNR of the kV-only inserts, respectively). In the kV-MV MAR reconstructions, streaking artifacts were substantially reduced with all inserts becoming clearly visible in the kV/CWO image while only two were visible in the kV/Cu-GOS image (average SNRs of the kV/CWO and kV/Cu-GOS CIRS with metal inserts were 0.94× and 0.35× the SNRs of the kV-only CIRS without metal inserts).

CONCLUSIONS

We have demonstrated that a high-DQE MV detector can be applied to generating high-quality combined kV-MV images for SRT and MAR. Clinically acceptable doses were utilized.

摘要

目的

联合千伏-兆伏锥形束 CT(CBCT)成像已经被提出用于两个潜在重要的图像引导放射治疗应用:(a)扫描时间减少(STR)和(b)金属伪影减少(MAR)。然而,由于商业电子射野影像系统(EPID)的量子探测效率(DQE)较低,这些技术的可行性一直存在疑问。这项工作的目的是测试一种高 DQE MV 探测器是否可以在可接受的剂量水平下生成可接受质量的预处理 CBCT 图像。

方法

在 Truebeam 系统(Varian,Palo Alto,CA)上获取 6MV 和 100kVp 投影数据。MV 数据是使用包含两个闪烁器的原型 EPID 采集的:(a)一种标准的铜-钆氧硫化物(Cu-GOS)屏幕,具有零频率 DQE(DQE(0))值为 1.4%,和(b)一个原型聚焦的镉钨酸盐(CWO)像素化“条带”,DQE(0) = 22%。kV 数据是使用标准的内置成像器采集的(DQE(0) = 70%)。MV 投影的角间距为 0.81°,源输出为 0.03MU/投影,而 kV 投影以 0.3mAs/投影的角间距 0.4°采集。使用(a)带有九个对比度插入物的 18cm 直径电子密度体模(CIRS,Norfolk,VA)和(b)20cm 直径 Catphan 体模的分辨率部分(The Phantom Laboratory,Greenwich,NY)评估图像质量。对于 MAR 研究,用钢棒代替两个相对的 CIRS 体模插入物。重建方法基于将 MV 和 kV 数据合并到一个 sinogram 中。MAR 重建主要使用 kV 原始数据,只有那些被金属损坏的射线需要用 MV 数据替换(总吸收剂量=0.7cGy)。对于 STR 研究,将来自部分重叠的 105kV 和 MV 采集的投影组合在一起,创建一个可以在 18 秒内采集的完整数据集(吸收剂量=2.5cGy)。还重建了 MV 仅(4.3cGy)和 kV 仅(0.3cGy)图像。

结果

在 MV 仅 CWO 和 GOS CIRS 体模图像中,插入物的平均信噪比(SNR)分别是 kV 仅图像中插入物 SNR 的 0.62×和 0.12×。MV 仅 GOS、MV 仅 CWO 和 kV 仅 Catphan 图像的限制空间分辨率分别为 3、6 和 8lp/cm。在联合 kV/CWO STR 重建中,所有对比度插入物都可见,而在 kV/Cu-GOS 图像中,由于噪声水平较高,只有两个插入物可以检测到(kV/CWO 和 kV/Cu-GOS 插入物的平均 SNR 分别是 kV 仅插入物 SNR 的 0.97×和 0.18×)。在 kV-MV MAR 重建中,条纹伪影大大减少,所有插入物在 kV/CWO 图像中都清晰可见,而在 kV/Cu-GOS 图像中只有两个插入物可见(kV/CWO 和 kV/Cu-GOS CIRS 带有金属插入物的平均 SNR 分别是 kV 仅 CIRS 无金属插入物 SNR 的 0.94×和 0.35×)。

结论

我们已经证明,一种高 DQE MV 探测器可用于生成用于 SRT 和 MAR 的高质量联合 kV-MV 图像。使用了临床可接受的剂量。

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