利用超声穿越时间光谱法测量松质骨的背向散射。

Yan Jia, Shuai Han, Boyi Li, Chengcheng Liu, Dean Ta
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摘要

最近,超声穿越时间光谱法(UTTS)作为一种有前途的骨定量超声测量方法被提出。研究表明,UTTS 可以在超声穿透测量中估算骨体积分数和其他骨小梁结构。本研究的目的是探索将UTTS应用于超声后向散射测量的可行性,并进一步评估后向散射超声传输时间谱(BS-UTTS)在松质骨密度和结构测量中的性能。首先,考虑到超声衰减,在一组不同位置和强度的散射体模拟的超声后向散射信号上验证了 BS-UTTS 的概念。然后,对 26 块牛松质骨标本进行了体外反向散射测量。在对 BS-UTTS 进行对数压缩后,将对数压缩后的 BS-UTTS 与超声波传播距离进行线性拟合,并确定 BS-UTTS 拟合线的斜率和截距。使用简单线性回归分析了 BS-UTTS 参数与松质骨特征之间的关联。结果表明,即使模拟的后向散射信号信噪比相对较低,BS-UTTS 也能对后向散射信号进行精确解卷积,并预测模拟散射体的位置和强度,消除了相位干扰。随着散射体位置和强度的变化,对数压缩 BS-UTTS 与超声波传播距离的拟合线斜率(简称 BS-UTTS 斜率)与模拟反向散射信号中的超声波衰减具有很高的一致性(r2 = 99.84%-99.96%)。与高密度松质骨相比,低密度试样在 BS-UTTS 中表现出更丰富的反向散射脉冲响应。BS-UTTS 的斜率与骨矿物质密度(r = 0.87;p < 0.001)、BV/TV(r = 0.87;p < 0.001)和松质骨微结构(r 高达 0.87;p < 0.05)显著相关。BS-UTTS 的截距也与骨密度 (r = -0.87; p < 0.001) 和骨小梁结构 (|r|=0.43-0.80; p < 0.05) 显著相关。然而,在进行实验测量时,BS-UTTS 的斜率低估了衰减。此外,在测量的衰减量与 BS-UTTS 斜率估算的衰减量之间存在明显的非线性关系。这项研究表明,UTTS 方法可用于松质骨的超声反向散射测量。得出的 BS-UTTS 斜率和截距可用于测量骨密度和微观结构。后向散射超声透过时间光谱法在临床诊断骨质疏松症方面可能具有潜力。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Backscatter measurement of cancellous bone using the ultrasound transit time spectroscopy.
Recently, ultrasound transit time spectroscopy (UTTS) was proposed as a promising method for bone quantitative ultrasound measurement. Studies have showed that UTTS could estimate the bone volume fraction and other trabecular bone structure in ultrasonic through-transmission measurements. The goal of this study was to explore the feasibility of UTTS to be adapted in ultrasonic backscatter measurement and further evaluate the performance of backscattered ultrasound transit time spectrum (BS-UTTS) in the measurement of cancellous bone density and structure. First, taking ultrasonic attenuation into account, the concept of BS-UTTS was verified on ultrasonic backscatter signals simulated from a set of scatterers with different positions and intensities. Then, in vitro backscatter measurements were performed on 26 bovine cancellous bone specimens. After a logarithmic compression of the BS-UTTS, a linear fitting of the log-compressed BS-UTTS versus ultrasonic propagated distance was performed and the slope and intercept of the fitted line for BS-UTTS were determined. The associations between BS-UTTS parameters and cancellous bone features were analyzed using simple linear regression. The results showed that the BS-UTTS could make an accurate deconvolution of the backscatter signal and predict the position and intensity of the simulated scatterers eliminating phase interference, even the simulated backscatter signal was with a relatively low signal-to-noise ratio. With varied positions and intensities of the scatterers, the slope of the fitted line for the log-compressed BS-UTTS versus ultrasonic propagated distance (i.e., slope of BS-UTTS for short) yield a high agreement (r2 = 99.84%-99.96%) with ultrasonic attenuation in simulated backscatter signal. Compared with the high-density cancellous bone, the low-density specimen showed more abundant backscatter impulse response in the BS-UTTS. The slope of BS-UTTS yield a significant correlation with bone mineral density (r = 0.87; p < 0.001), BV/TV (r = 0.87; p < 0.001), and cancellous bone microstructures (r up to 0.87; p < 0.05). The intercept of BS-UTTS was also significantly correlated with bone densities (r = -0.87; p < 0.001) and trabecular structures (|r|=0.43-0.80; p < 0.05). However, the slope of the BS-UTTS underestimated attenuation when measurements were performed experimentally. In addition, a significant non-linear relationship was observed between the measured attenuation and the attenuation estimated by the slope of the BS-UTTS. This study demonstrated that the UTTS method could be adapted to ultrasonic backscatter measurement of cancellous bone. The derived slope and intercept of BS-UTTS could be used in the measurement of bone density and microstructure. The backscattered ultrasound transit time spectroscopy might have potential in the diagnosis of osteoporosis in the clinic.
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