Department of Medical Biophysics, University of Toronto, Toronto, Ontario M5G 2M9, Canada and Radiation Medicine Program, Princess Margaret Hospital, Toronto, Ontario M5G 2M9, Canada.
Med Phys. 2013 Nov;40(11):111901. doi: 10.1118/1.4822484.
X-ray scatter is a source of significant image quality loss in cone-beam computed tomography (CBCT). The use of Monte Carlo (MC) simulations separating primary and scattered photons has allowed the structure and nature of the scatter distribution in CBCT to become better elucidated. This work seeks to quantify the structure and determine a suitable basis function for the scatter distribution by examining its spectral components using Fourier analysis.
The scatter distribution projection data were simulated using a CBCT MC model based on the EGSnrc code. CBCT projection data, with separated primary and scatter signal, were generated for a 30.6 cm diameter water cylinder [single angle projection with varying axis-to-detector distance (ADD) and bowtie filters] and two anthropomorphic phantoms (head and pelvis, 360 projections sampled every 1°, with and without a compensator). The Fourier transform of the resulting scatter distributions was computed and analyzed both qualitatively and quantitatively. A novel metric called the scatter frequency width (SFW) is introduced to determine the scatter distribution's frequency content. The frequency content results are used to determine a set basis functions, consisting of low-frequency sine and cosine functions, to fit and denoise the scatter distribution generated from MC simulations using a reduced number of photons and projections. The signal recovery is implemented using Fourier filtering (low-pass Butterworth filter) and interpolation. Estimates of the scatter distribution are used to correct and reconstruct simulated projections.
The spatial and angular frequencies are contained within a maximum frequency of 0.1 cm(-1) and 7/(2π) rad(-1) for the imaging scenarios examined, with these values varying depending on the object and imaging setup (e.g., ADD and compensator). These data indicate spatial and angular sampling every 5 cm and π/7 rad (~25°) can be used to properly capture the scatter distribution, with reduced sampling possible depending on the imaging scenario. Using a low-pass Butterworth filter, tuned with the SFW values, to denoise the scatter projection data generated from MC simulations using 10(6) photons resulted in an error reduction of greater than 85% for the estimating scatter in single and multiple projections. Analysis showed that the use of a compensator helped reduce the error in estimating the scatter distribution from limited photon simulations by more than 37% when compared to the case without a compensator for the head and pelvis phantoms. Reconstructions of simulated head phantom projections corrected by the filtered and interpolated scatter estimates showed improvements in overall image quality.
The spatial frequency content of the scatter distribution in CBCT is found to be contained within the low frequency domain. The frequency content is modulated both by object and imaging parameters (ADD and compensator). The low-frequency nature of the scatter distribution allows for a limited set of sine and cosine basis functions to be used to accurately represent the scatter signal in the presence of noise and reduced data sampling decreasing MC based scatter estimation time. Compensator induced modulation of the scatter distribution reduces the frequency content and improves the fitting results.
在锥束计算机断层扫描(CBCT)中,X 射线散射是图像质量严重损失的一个来源。使用蒙特卡罗(MC)模拟分离初级和散射光子,使 CBCT 中散射分布的结构和性质得到了更好的阐明。本研究旨在通过傅里叶分析检查其光谱分量来量化结构并确定散射分布的合适基函数。
使用基于 EGSnrc 代码的 CBCT MC 模型模拟散射分布投影数据。为 30.6cm 直径的水筒(单角度投影,轴与探测器距离(ADD)和蝴蝶结滤光器变化)和两个人体模型(头部和骨盆,360 个投影,每 1°采样一次,有和没有补偿器)生成了带有分离的初级和散射信号的 CBCT 投影数据。对得到的散射分布进行傅里叶变换,从定性和定量两方面进行分析。引入了一个新的度量标准,即散射频率宽度(SFW),用于确定散射分布的频率内容。频率内容的结果用于确定一组基函数,包括低频正弦和余弦函数,以使用较少的光子和投影来拟合和降噪从 MC 模拟生成的散射分布。使用傅里叶滤波(低通巴特沃斯滤波器)和插值来实现信号恢复。使用估计的散射分布来校正和重建模拟投影。
在所研究的成像场景中,空间和角频率包含在 0.1cm(-1)和 7/(2π)rad(-1)的最大频率内,这些值随物体和成像设置(如 ADD 和补偿器)而变化。这些数据表明,空间和角采样间隔为 5cm 和 π/7rad(~25°)可以正确捕获散射分布,根据成像场景,采样间隔可以减小。使用低通巴特沃斯滤波器,根据 SFW 值进行调谐,对使用 10(6)个光子从 MC 模拟生成的散射投影数据进行降噪处理,可将单投影和多投影中散射估计的误差减少 85%以上。分析表明,与没有补偿器的情况相比,使用补偿器可以帮助减少有限光子模拟中估计散射分布的误差,对于头部和骨盆模型,补偿器的使用可以减少超过 37%的误差。通过过滤和插值的散射估计校正的模拟头部模型投影的重建显示出整体图像质量的提高。
在 CBCT 中,散射分布的空间频率内容被发现包含在低频域内。频率内容既受物体又受成像参数(ADD 和补偿器)的调制。散射分布的低频特性允许使用有限的正弦和余弦基函数来准确表示存在噪声和减少数据采样时的散射信号,从而减少基于 MC 的散射估计时间。补偿器引起的散射分布调制降低了频率内容并改善了拟合结果。